Ultrasonic motor, drive control system, optical apparatus, and vibrator

ABSTRACT

An ultrasonic motor, usable in a drive control system and the like, includes an annular vibrator and an annular moving member arranged so as to be brought into pressure-contact with the vibrator. The vibrator includes an annular vibrating plate and an annular piezoelectric element. The piezoelectric element includes an annular piezoelectric ceramic piece, a common electrode arranged on one surface of the piezoelectric ceramic piece, and a plurality of electrodes arranged on the other surface of the piezoelectric ceramic piece. The piezoelectric ceramic piece contains lead in a content of less than 1,000 ppm. The plurality of electrodes include two drive phase electrodes, one or more non-drive phase electrodes, and one or more detection phase electrodes.

BACKGROUND OF THE INVENTION

Field of the Invention

The present invention relates to an ultrasonic motor, a drive control system and an optical apparatus that use the ultrasonic motor, and further, to a vibrator to be used in the ultrasonic motor.

Description of the Related Art

A vibration-type (vibrational wave) actuator includes a vibrator configured to excite vibration in an elastic body having an annular shape, an elliptical shape, a bar shape, or the like, which is joined to an electromechanical energy converting element, e.g., a piezoelectric element, by applying an electric signal, e.g., alternating voltage to the electromechanical energy converting element. The vibration-type actuator is used, for example, as an ultrasonic motor configured to relatively move an elastic body (moving member) that is brought into pressure-contact with the vibrator and the vibrator (static member) through use of the drive force of the vibration excited in the vibrator.

Now, an overview of the structure and drive principle of an annular ultrasonic motor that is a typical usage form of the vibration-type actuator is described. In the following description, the term “annular” is intended to mean that an annular article or element can be schematically regarded as a configuration in which a disc having a predetermined thickness includes a circular through hole concentrically. In this case, the dimension of the disc-shaped article or element corresponding to the thickness of the disc is referred to as “thickness” of the article or element, and respective surfaces of the annular article or element corresponding to both surfaces of the disc that hold the thickness of the disc are individually or generically referred to as “surfaces” of the article or element.

The annular ultrasonic motor includes an annular vibrator and an annular moving member that is brought into pressure-contact with the vibrator. The moving member is formed of an elastic body, and a metal is generally used as a material for the moving member. The vibrator includes an annular vibrating plate and an annular piezoelectric element arranged on one surface of the vibrating plate. The vibrating plate is formed of an elastic body, and a metal is generally used as a material for the vibrating plate. The piezoelectric element includes, on one surface of an annular piezoelectric ceramics, an electrode divided into a plurality of regions along the circumferential direction of the annular ring and one common electrode on the other surface thereof. A lead zirconate titanate-based material is generally used as a material for the piezoelectric ceramics.

The electrode divided into a plurality of regions includes two regions forming drive phase electrodes, at least one region forming a detection phase electrode, and a region forming a non-drive phase electrode, which is arranged as necessary. Wiring configured to input electric power for applying an electric field to a corresponding region of the annular piezoelectric ceramics that is brought into contact with each drive phase electrode is arranged in each drive phase electrode, and the wiring is connected to a power source unit.

A circle that passes through an arbitrary position on the surface of the annular piezoelectric element and shares the center with the annular ring is assumed, and the length of one arc obtained by dividing the circumference of the circle by n (n is a natural number) is represented by λ, and the circumferential length of the circle is represented by nλ. A region of the piezoelectric ceramics corresponding to the region forming each drive phase electrode is subjected to polarization treatment in advance by applying an electric field to the piezoelectric ceramics in a thickness direction thereof alternately in an opposite direction at a pitch of λ/2 along the circumferential direction. Therefore, when an electric field in the same direction is applied to the piezoelectric ceramics in the thickness direction with respect to all the regions, the expansion and contraction polarity of the piezoelectric ceramics in the regions is reversed alternately at a pitch of λ/2. The two regions forming the respective drive phase electrodes are arranged at a distance of an odd multiple of λ/4 in the circumferential direction. In general, two regions (spacing regions) that separate the two drive phase electrodes from each other include non-drive phase electrodes that are short-circuited to a common electrode so that piezoelectric vibration is not caused spontaneously, with the result that an electric field is not applied to the piezoelectric ceramics in those regions. In general, a detection phase electrode is arranged in the spacing region as described later.

When an alternating voltage is applied to only one of the drive phase electrodes of such an ultrasonic motor, a first standing wave having a wavelength λ is generated over the entire circumference of the vibrator. When an alternating voltage is applied to only the other drive phase electrode, a second standing wave is generated similarly, but the position of the wave is rotated and moved by λ/4 in the circumferential direction with respect to the first standing wave. Meanwhile, when alternating voltages, which have the same frequency and a temporal phase difference of π/2, are applied to the respective drive phase electrodes, a propagating wave (wave number along the annular ring: n and wavelength: λ) of bending vibration (vibration having an amplitude perpendicular to the surface of the vibrator), which propagates in the circumferential direction over the entire circumference, is generated in the vibrator as a result of the synthesis of both the standing waves.

When the propagating wave of the bending vibration (hereinafter sometimes simply referred to as “bending vibration wave”) is generated, each point on the surface of the vibrating plate forming the vibrator undergoes an elliptical motion. Therefore, the moving member that is brought into contact with the surface rotates due to friction force (drive force) in the circumferential direction from the vibrating plate. The rotation direction can be reversed by switching, between positive and negative, a phase difference π/2 of the alternating voltage applied to each drive phase electrode. Further, the rotation speed can be controlled by changing the frequency and amplitude of the alternating voltage applied to each drive phase electrode.

The generated bending vibration wave can be detected with the detection phase electrode arranged in the spacing region. That is, the distortion of deformation (vibration) generated in the piezoelectric ceramics brought into contact with the detection phase electrode is converted into an electric signal in accordance with the magnitude of the distortion and output to a drive circuit through the detection phase electrode.

When an alternating voltage is applied to the ultrasonic motor at a frequency higher than a resonant frequency, the ultrasonic motor starts a rotation operation. When the frequency is brought close to the resonant frequency, the rotation is accelerated to reach a highest rotation speed at the resonant frequency. Thus, the ultrasonic motor is generally driven at a desired rotation speed by sweeping the frequency from a frequency region higher than the resonant frequency to the resonant frequency.

Meanwhile, a lead zirconate titanate-based material to be used as a material for the piezoelectric ceramics contains a large amount of lead in an A-site of an ABO₃ perovskite type metal oxide. Accordingly, an effect of a lead component on environments has been seen as a problem. In order to deal with this problem, piezoelectric ceramics using a perovskite type metal oxide that does not contain lead (lead content is smaller than 1,000 ppm) has been proposed.

In Japanese Patent No. 5344456, there is disclosed piezoelectric ceramics in which piezoelectric characteristics are enhanced by substituting a part of an A-site of barium titanate with calcium (Ca) and substituting a part of a B-site thereof with zirconium (Zr). In Japanese Patent No. 5213135, there is disclosed piezoelectric ceramics containing (Na,K)NbO₃ as a main component, in which piezoelectric characteristics are enhanced through use of a boundary of a rhombohedral phase and a tetragonal phase.

In recent years, the function of moving a weight body, e.g., a super-telephoto lens with an ultrasonic motor is becoming necessary. However, with the piezoelectric ceramics disclosed in Japanese Patent Nos. 5344456 and 5213135, even when an attempt is made to move a body with a high load, e.g., a super-telephoto lens by manufacturing an ultrasonic motor through use of a related-art vibrator, the rotation speed of a sufficient ultrasonic motor cannot be obtained due to the shortage of torque.

SUMMARY OF THE INVENTION

The present invention has been made to solve the above-mentioned problems, and it is an object of the present invention to provide an ultrasonic motor configured to be rotated with sufficient torque even when lead-free piezoelectric ceramics is used. It is also an object of the present invention to provide a drive control system and an optical apparatus that use the ultrasonic motor, and a vibrator to be used in the ultrasonic motor.

In order to solve the above-mentioned problems, according to one embodiment of the present invention, there is provided an ultrasonic motor, including: an annular vibrator; and an annular moving member arranged so as to be brought into pressure-contact with the annular vibrator, in which the annular vibrator includes: an annular vibrating plate; and an annular piezoelectric element arranged on a first surface of the annular vibrating plate, the annular vibrating plate being brought into contact with the annular moving member on a second surface on a side opposite to the first surface, in which the annular piezoelectric element includes: an annular piezoelectric ceramic piece; a common electrode arranged on a surface of the annular piezoelectric ceramic piece opposed to the annular vibrating plate so as to be sandwiched between the annular piezoelectric ceramic piece and the annular vibrating plate; and a plurality of electrodes arranged on a surface of the annular piezoelectric ceramic piece on a side opposite to the surface on which the common electrode is arranged, in which the annular piezoelectric ceramic piece contains lead in a content of less than 1,000 ppm, in which the plurality of electrodes include two drive phase electrodes, one or more non-drive phase electrodes, and one or more detection phase electrodes, in which the second surface of the annular vibrating plate includes groove regions extending radially in X portions, and when an outer diameter of the annular vibrating plate is set to 2R in a unit of mm, the X is a natural number satisfying ((2R/0.85)−5)≤X≤((2R/0.85)+15) and the outer diameter 2R is 57 mm or more, in which a ratio between an average value L_(top) of a length in a circumferential direction on an outer diameter side of a wall region that separates the adjacent groove regions from each other and an average value L_(btm) of a length in a circumferential direction on an outer diameter side of the groove regions falls within a range of 2.00≤L_(top)/L_(btm)≤2.86, and in which, when center depths of the groove regions in the X portions are represented by D₁ to D_(X) in order in the circumferential direction, D₁ to D_(X) change so as to follow a curve obtained by superimposing one or more sine waves on one another, the groove regions reaching a local maximum in 12 or more regions in the change of the center depth and the groove regions reaching a local minimum in 12 or more regions in the change of the center depth, the groove regions reaching the local maximum and the groove regions reaching the local minimum being prevented from being adjacent to each other.

In order to solve the above-mentioned problems, according to another embodiment of the present invention, there is provided a drive control system, including at least the above-mentioned ultrasonic motor and a drive circuit electrically connected to the ultrasonic motor.

In order to solve the above-mentioned problems, according to still another embodiment of the present invention, there is provided an optical apparatus, including at least the above-mentioned drive control system and an optical element dynamically connected to the ultrasonic motor.

In order to solve the above-mentioned problems, according to yet another embodiment of the present invention, there is provided an annular vibrator, including: an annular vibrating plate; and an annular piezoelectric element arranged on a first surface of the annular vibrating plate, in which the annular piezoelectric element includes: an annular piezoelectric ceramic piece; a common electrode arranged on a surface of the annular piezoelectric ceramic piece opposed to the annular vibrating plate so as to be sandwiched between the annular piezoelectric ceramic piece and the annular vibrating plate; and a plurality of electrodes arranged on a surface of the annular piezoelectric ceramic piece on a side opposite to the surface on which the common electrode is arranged, in which the annular piezoelectric ceramic piece contains lead in a content of less than 1,000 ppm, in which the plurality of electrodes include two drive phase electrodes, one or more non-drive phase electrodes, and one or more detection phase electrodes, in which a second surface of the annular vibrating plate includes groove regions extending radially in X portions, and when an outer diameter of the annular vibrating plate is set to 2R in a unit of mm, X is a natural number satisfying ((2R/0.85)−5)≤X≤((2R/0.85)+15) and the outer diameter 2R is 57 mm or more, in which a ratio between an average value L_(top) of a length in a circumferential direction on an outer diameter side of a wall region that separates the adjacent groove regions and an average value L_(btm) of a length in a circumferential direction on an outer diameter side of the groove regions falls within a range of 2.00≤L_(top)/L_(btm)≤2.86, and in which, when center depths of the groove regions in the X portions are represented by D₁ to D_(X) in order in the circumferential direction, D₁ to D_(X) change so as to follow a curve obtained by superimposing one or more sine waves on one another, the groove regions reaching a local maximum in 12 or more regions in the change of the center depth and the groove regions reaching a local minimum in 12 or more regions in the change of the center depth, the groove regions reaching the local maximum and the groove regions reaching the local minimum being prevented from being adjacent to each other.

According to the present invention, in the ultrasonic motor using the lead-free piezoelectric ceramics or the drive control system and the optical apparatus that use the ultrasonic motor, a sufficient drive speed can be exhibited even when a high load (for example, 500 gf·cm or more) is applied.

Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A and FIG. 1B are each a schematic view for illustrating an ultrasonic motor according to an embodiment of the present invention.

FIG. 2 is a schematic sectional view for illustrating a part of a configuration of the ultrasonic motor according to the embodiment of the present invention.

FIG. 3 is a schematic view for illustrating a relationship between a circumferential length and the wavelength of a vibration wave in an annular piezoelectric element to be used in the ultrasonic motor and a vibrator of the present invention.

FIG. 4A and FIG. 4B are each a schematic view of the annular piezoelectric element to be used in the ultrasonic motor and the vibrator according to an embodiment of the present invention.

FIG. 5 is a graph for showing a relationship between the number of protrusion regions and groove regions, and the outer diameter of an annular vibrating plate to be used in the ultrasonic motor and the vibrator of the present invention.

FIG. 6A, FIG. 6B, FIG. 6C, and FIG. 6D are each a schematic view for illustrating a method of measuring a length in a circumferential direction on an outer diameter side of the protrusion region and the groove region of the annular vibrating plate to be used in the ultrasonic motor and the vibrator of the present invention.

FIG. 7A, FIG. 7B, FIG. 7C, and FIG. 7D are each a graph for schematically showing a distribution of a center depth of the groove regions of the vibrating plate of the ultrasonic motor and the vibrator according to the embodiment of the present invention.

FIG. 7E, FIG. 7F, FIG. 7G, and FIG. 7H are each a graph for schematically showing a distribution of a center depth of the groove regions of the vibrating plate of the ultrasonic motor and the vibrator according to the embodiment of the present invention.

FIG. 8 is a schematic view for illustrating a drive control system according to an embodiment of the present invention.

FIG. 9A and FIG. 9B are each a schematic view for illustrating an optical apparatus according to an embodiment of the present invention.

FIG. 10 is a schematic view for illustrating an optical apparatus according to the embodiment of the present invention.

FIG. 11A and FIG. 11B are each a schematic step view for illustrating an example of a manufacturing process of the annular vibrating plate to be used in the ultrasonic motor and the vibrator of the present invention.

FIG. 12A, FIG. 12B, FIG. 12C, FIG. 12D, and FIG. 12E are each a schematic step view for illustrating an example of a manufacturing process of the ultrasonic motor of the present invention.

DESCRIPTION OF THE EMBODIMENTS

Preferred embodiments of the present invention will now be described in detail in accordance with the accompanying drawings.

Now, an ultrasonic motor, a drive control system, an optical apparatus, and a vibrator according to embodiments of the present invention for carrying out the present invention are described.

(Ultrasonic Motor and Vibrator that can be Used in Ultrasonic Motor)

The ultrasonic motor of the present invention has the following features. The ultrasonic motor includes an annular vibrator and an annular moving member that is arranged so as to be brought into pressure-contact with the vibrator. The vibrator includes an annular vibrating plate and an annular piezoelectric element arranged on a first surface (one surface) of the vibrating plate, a second surface (surface on a side opposite to the first surface) of the vibrating plate being brought into contact with the moving member. The piezoelectric element includes an annular piezoelectric ceramic piece (formed in an integrated manner without seams), a common electrode arranged on one surface (on a surface opposed to the vibrating plate) of the piezoelectric ceramic piece, and a plurality of electrodes arranged on the other surface (on a side opposite to the surface on which the common electrode is arranged) of the piezoelectric ceramic piece. The piezoelectric ceramic piece contains lead in a content of less than 1,000 ppm. The plurality of electrodes include two drive phase electrodes, one or more non-drive phase electrodes, and one or more detection phase electrodes. A second surface of the annular vibrating plate includes groove regions extending radially in X portions. At this time, X is a natural number satisfying 2R/0.85−5≤X≤2R/0.85+15 (2R is the outer diameter of the vibrating plate; unit: mm), 2R is 57 mm or more, and a ratio between an average value L_(top) of a length in a circumferential direction on an outer diameter side of a wall region that separates the adjacent groove regions from each other and an average value L_(btm) of a length in a circumferential direction on an outer diameter side of the groove regions falls within a range of 2.00≤L_(top)/L_(btm)≤2.86. When center depths of the groove regions in the X portions are represented by D₁ to D_(X) in order in the circumferential direction, the D₁ to the D_(X) change so as to follow a curve obtained by superimposing one or more sine waves on one another, the groove regions reaching a local maximum in 12 or more regions in the change of the center depth and the groove regions reaching a local minimum in 12 or more regions in the change of the center depth, the groove regions reaching the local maximum and the groove regions reaching the local minimum being prevented from being adjacent to each other.

The ultrasonic motor of the present invention can exhibit a sufficient drive speed with high torque even in a high load by satisfying the above-mentioned condition. The ultrasonic motor of the present invention can also remove unnecessary vibration waves that do not contribute to drive so as to be driven with satisfactory efficiency (efficiency of an output with respect to input power to the ultrasonic motor) while exhibiting a sufficient drive speed with high torque.

(FIG. 1A and FIG. 1B, and FIG. 2)

The ultrasonic motor of the present invention includes an annular vibrator 1 and an annular moving member 2 arranged so as to be in contact with the vibrator 1.

FIG. 1A and FIG. 1B are each a schematic view for illustrating the ultrasonic motor according to an embodiment of the present invention. FIG. 1A is a schematic perspective view of the ultrasonic motor when viewed from an oblique direction, and FIG. 1B is a schematic plan view of the ultrasonic motor when viewed from a side on which a plurality of electrodes (pattern electrodes) are arranged.

FIG. 2 is a schematic partial sectional view of a detailed configuration of the ultrasonic motor according to the embodiment of the present invention when viewed from a side direction. The side direction as used herein refers to a position away from the annular ring in a radial direction.

(Annular Shape)

In the present invention, as described above, the annular shape refers to a shape in which a disc having a predetermined thickness can be schematically regarded as a configuration that includes a circular through hole concentrically. The outer peripheral shapes of the disc and the through hole are ideally true circular shapes, but include an oval shape, an elliptical shape, and the like as long as the shape can be schematically regarded as an annular ring. The radius and diameter when the circular shape is not a true circular shape are determined assuming a true circle having the same area. A substantially annular shape, such as a shape in which a part of an annular ring is chipped, a shape in which a part of an annular ring is cut, or a shape in which a part of an annular ring protrudes, is also included in the annular shape in the present invention as long as the substantially annular shape can be substantially regarded as an annular shape. Thus, a substantially annular shape that is slightly deformed due to the variation in manufacturing is also included in the annular shape in the present invention as long as the substantially annular shape can be substantially regarded as an annular shape. The radius and diameter when the circular shape is a substantially annular shape are determined assuming a true circle in which a defective region and an abnormal region are corrected.

(Moving Member)

The annular moving member 2 is similarly brought into pressure-contact with the annular vibrator 1 and rotates by the drive force caused by the vibration generated in a contact surface with respect to the vibrator 1. It is preferred that the contact surface of the moving member 2 with respect to the vibrator 1 be flat (even). It is preferred that the moving member 2 be formed of an elastic body, and a material for the moving member 2 be a metal. For example, aluminum is used suitably as the material for the moving member 2. The surface of the aluminum may be subjected to alumite (anodization) treatment.

(Vibrator)

As illustrated in FIG. 1A, the vibrator 1 includes an annular vibrating plate 101 and an annular piezoelectric element 102 arranged on a first surface of the vibrating plate 101 and is brought into contact with the moving member 2 on a second surface of the vibrating plate 101.

It is preferred that the moving member 2 be pressed against the second surface of the vibrating plate 101 by appropriate external force so that the transmission of the drive force from the vibrator 1 to the moving member 2 becomes more satisfactory.

An outer diameter 2R (unit: mm) of the vibrating plate 101 is 57 mm or more (2R≥57). When the outer diameter 2R is smaller than 57 mm, a region of the through hole becomes smaller, and hence the advantage of the annular ring may not be obtained. It is not practically suitable that the outer diameter be small, for example, in the case of using the ultrasonic motor of the present invention for the purpose of moving a lens for a camera so that the area through which a light flux passes becomes smaller.

There is no particular limitation on the upper limit of the outer diameter 2R of the vibrating plate 101, but from the viewpoint that unnecessary vibration waves that do not contribute to drive can be sufficiently removed, it is preferred that a relationship: 2R≤90 mm be satisfied. It is more preferred that a relationship: 2R≤80 mm be satisfied. When the outer peripheral surface of the vibrating plate 101 does not have a simple shape and has a plurality of outer diameters depending on a measurement position, the maximum outer diameter is set to 2R.

There is no particular limitation on an inner diameter 2R_(in) (unit: mm) of the vibrating plate 101 as long as the inner diameter 2R_(in) is smaller than the outer diameter 2R, but it is preferred that a relationship: 2R-16≤2R_(in)≤2R−6 be satisfied. This requirement can be interpreted as setting a length in a radial direction of the annular ring of the vibrating plate 101 (hereinafter referred to as “width” of the annular ring) to 3 mm or more and 8 mm or less. When the width of the annular ring of the vibrating plate 101 is set to within the above-mentioned range, sufficient drive force is generated during drive of the ultrasonic motor while the advantage of the annular shape is ensured. When the inner diameter 2R_(in) is smaller than 2R−16, a region of the through hole becomes smaller. Therefore, the advantage of the annular ring may not be obtained as described above. Meanwhile, when 2R_(in) is larger than 2R−6, the width of the annular ring of the vibrating plate 101 becomes insufficient, and there is a risk in that the drive force generated during drive of the ultrasonic motor may become insufficient. The drive force is substantially proportional to the piezoelectric constant, the Young's modulus, and the thickness of the annular ring. When the drive force increases, the moving member can be rotated at high speed even when the load of the moving member is large.

It is preferred that the first surface of the vibrating plate 101 be flat so that the transmission of vibration involved in the expansion and contraction of the piezoelectric element 102 becomes more satisfactory. It is preferred that the center of the annular ring of the vibrating plate 101 be matched with the center of the annular ring of the piezoelectric element 102 so that the transmission of vibration becomes more satisfactory.

There is no particular limitation on a method of arranging the piezoelectric element 102 on the first surface of the vibrating plate 101, but it is preferred to cause the piezoelectric element 102 to directly adhere to the first surface of the vibrating plate 101 so as not to inhibit the transmission of vibration or to cause the piezoelectric element 102 to adhere to the first surface of the vibrating plate 101 through intermediation of a highly-elastic material (not shown). When an adhesive layer (not shown) having a Young's modulus at room temperature (e.g., 20° C.) of 0.5 GPa or more, more preferably 1 GPa or more is arranged as an example of the highly-elastic material, the transmission of vibration from the piezoelectric element 102 to the vibrating plate 101 becomes more satisfactory. Meanwhile, the upper limit of the Young's modulus at room temperature of the adhesive layer may not be set particularly, but in order to sufficiently obtain adhesion strength of a resin after curing, the upper limit of the Young's modulus is preferably 10 GPa or less. For example, an epoxy resin is suitably used as the adhesive layer. The Young's modulus at room temperature of the adhesive layer can be calculated by JIS K6911 “General test methods for thermosetting plastics” (1995).

The maximum thickness of the vibrating plate 101 is represented by T_(dia) (unit: mm). As the maximum thickness of the vibrating plate 101, a distance between the first surface of the vibrating plate 101 and a top surface of a protrusion region 1011 is generally taken. When the thickness of the vibrating plate 101 varies depending on the position, the maximum value is basically defined as the maximum thickness of the vibrating plate 101.

It is preferred that the maximum thickness T_(dia) be 4 mm or more and 6 mm or less. When the maximum thickness T_(dia) is smaller than 4 mm, a neutral surface of elastic deformation (distortion) as the vibrator 1 is shifted to a piezoelectric ceramic piece 1021 side, and hence the efficiency of motor drive is degraded. When the piezoelectric ceramic piece 1021 is decreased in thickness for the purpose of returning the neutral surface to the vibrating plate 101 side, a stress during deformation increases in proportion to an inverse square of the thickness, and hence the piezoelectric ceramic piece 1021 is liable to crack. Further, the generation force of the vibrator 1 decreases. Meanwhile, when the maximum thickness T_(dia) is larger than 6 mm, the deformation amount during motor drive of the vibrating plate 101 becomes smaller, and the rotation speed of the motor decreases. When the piezoelectric ceramic piece 1021 is increased in thickness for the purpose of compensating for the deformation amount during motor drive of the vibrating plate 101, the drive voltage of the motor increases excessively.

(Material for Vibrating Plate)

It is preferred that the vibrating plate 101 be formed of an elastic body for the purpose of forming a propagating wave of bending vibration together with the piezoelectric element 102 and transmitting the vibration to the moving member 2. It is preferred that the vibrating plate 101 be made of a metal from the viewpoint of the properties and processability of the elastic body. As the metal that can be used as the vibrating plate 101, there may be given aluminum, brass, a Fe—Ni 36% alloy, and stainless steel. Of those, stainless steel is preferably used in the present invention because stainless steel can provide a high rotation speed in combination with the piezoelectric ceramic piece 1021 having a Young's modulus at room temperature of 80 GPa or more and 125 GPa or less. Stainless steel as used herein refers to an alloy containing 50 mass % or more of steel and 10.5 mass % or more of chromium. Of the stainless steel, martensite stainless steel is preferred, and SUS420J2 is most preferred as a material for the vibrating plate 101.

(Piezoelectric Element)

As illustrated in FIG. 1A, the annular piezoelectric element 102 includes the annular piezoelectric ceramic piece 1021, a common electrode 1022 arranged on a surface of the piezoelectric ceramic piece 1021 opposed to the vibrating plate 101, and a plurality of electrodes 1023 arranged on a surface of the vibrating plate 101 on a side opposite to the surface on which the common electrode 1022 is arranged.

In the present invention, the piezoelectric ceramic piece 1021 is a bulk having a uniform composition, which is obtained by calcining raw material powder including metal elements, and refers to ceramics having an absolute value of a piezoelectric constant d₃₁ at room temperature of 10 pm/V or a piezoelectric constant d₃₃ at room temperature of 30 pC/N or more. The piezoelectric constant of piezoelectric ceramics can be determined by calculation based on the Japan Electronics and Information Technology Industries Association Standard (JEITA EM-4501) from the measurement results of a density, a resonant frequency, and an antiresonant frequency of the piezoelectric ceramics. This method is hereinafter referred to as a resonance-antiresonance method. The density can be measured, for example, by an Archimedes' method. The resonant frequency and the antiresonant frequency can be measured, for example, through use of an impedance analyzer.

Ceramics is generally an aggregate of fine crystals (also called “polycrystal”), and each crystal includes an atom having a positive charge and an atom having a negative charge. Most of the ceramics have a state in which the positive charge and the negative charge are balanced. However, dielectric ceramics also includes ceramics called ferroelectrics in which the positive charge and the negative charge in crystals are not balanced even in a natural state, and bias of charge (spontaneous polarization) occurs. The ferroelectric ceramics after calcination has spontaneous polarization in various directions and does not appear to have bias of charge in the entire ceramics. However, when a high voltage is applied to the ferroelectric ceramics, the directions of spontaneous polarization are aligned in a uniform direction, and the spontaneous polarization does not return to the original directions even when the voltage is removed. Aligning the directions of spontaneous polarization is generally called polarization treatment. When a voltage is applied to the ferroelectric ceramics subjected to the polarization treatment from outside, the centers of the respective positive and negative charges in the ceramics attract or repel external charge, and the ceramics main body expands or contracts (inverse piezoelectric effect). The piezoelectric ceramic piece 1021 of the present invention is subjected to such polarization treatment to cause the inverse piezoelectric effect, and at least a region of a part of the piezoelectric material piece is subjected to polarization treatment.

It is preferred that the outer diameter of the annular piezoelectric ceramic piece 1021 be smaller than the outer diameter 2R of the vibrating plate 101, and the inner diameter of the annular piezoelectric ceramic piece 1021 be larger than the inner diameter 2R_(in) of the vibrating plate 101. That is, it is preferred that, when the centers of the annular rings are matched, a projection surface of the piezoelectric ceramic piece 1021 in an annular ring center axial direction be included in a projection surface of the vibrating plate 101 in the same direction. When the outer diameter and the inner diameter of the annular piezoelectric ceramic piece 1021 are set to within such range, the transmission of vibration between the piezoelectric ceramic piece 1021 and the vibrating plate 101 becomes more satisfactory.

In the present invention, the piezoelectric ceramic piece 1021 contains lead in a content of less than 1,000 ppm. That is, the piezoelectric ceramic piece 1021 is lead-free piezoelectric ceramics. It is preferred that the piezoelectric ceramic piece 1021 have a Young's modulus at room temperature (e.g., 20° C.) of 80 GPa or more and 125 GPa or less. The Young's modulus at room temperature of the piezoelectric ceramic piece 1021 can be calculated by the above-mentioned resonance-antiresonance method. Most of the related-art piezoelectric ceramics contain lead zirconate titanate as a main component. Therefore, the following has been indicated. For example, when a piezoelectric element is discarded and exposed to acid rain or left in a severe environment, there is a risk in that a lead component in the related-art piezoelectric ceramics dissolves into the soil to cause harm to the ecosystem. However, when the content of lead is smaller than 1,000 ppm as in the piezoelectric ceramic piece 1021 of the present invention, for example, even when a piezoelectric element is discarded and exposed to acid rain or left in a severe environment, the influence of the lead component contained in the piezoelectric ceramic piece 1021 on the environment is negligible.

The content of lead contained in the piezoelectric ceramic piece 1021 can be evaluated based on the content of lead with respect to the total weight of the piezoelectric ceramic piece 1021, for example, quantified by X-ray fluorescence (XRF) analysis and ICP emission spectroscopic analysis.

When the Young's modulus at room temperature of the piezoelectric ceramic piece 1021 is smaller than 80 GPa, the drive force generated during drive of the ultrasonic motor may become insufficient. Meanwhile, when the Young's modulus at room temperature of the piezoelectric ceramics 1021 is larger than 125 GPa, the piezoelectric ceramic piece 1021 is liable to crack. For example, when the Young's modulus of the piezoelectric ceramic piece 1021 is large, the stress caused by deformation (distortion) of the piezoelectric ceramic piece 1021 occurring due to the drive of the ultrasonic motor increases, and hence there is a risk in that the piezoelectric ceramic piece 1021 is liable to crack. For example, when the Young's modulus is large, a neutral surface of elastic deformation as the vibrator 1 is shifted from the vibrating plate 101 side to the piezoelectric ceramic piece 1021 side. Therefore, the efficiency of the motor drive is degraded. In view of this, when the thickness of the piezoelectric ceramic piece 1021 is reduced so as to return the neutral surface to the vibrating plate 101 side, the stress during deformation increases in proportion to the inverse square of the thickness, and hence the piezoelectric ceramic piece 1021 is liable to crack. The preferred range of the Young's modulus at room temperature of the piezoelectric ceramic piece 1021 is 95 GPa or more and 125 GPa or less.

As a main component of the piezoelectric ceramic piece 1021 in which the content of lead is smaller than 1,000 ppm, and the Young's modulus at room temperature is GPa or more and 125 GPa or less, a metal oxide (perovskite type metal oxide) having a perovskite type crystal structure is preferred.

The perovskite type metal oxide of the present invention refers to a metal oxide having a perovskite structure that is ideally a cubic structure as described in “Iwanami Dictionary of Physics and Chemistry”, Fifth Edition (Iwanami Shoten, published on Feb. 20, 1998). The metal oxide having a perovskite structure is generally represented by a chemical formula of ABO₃. Although the molar ratio between the element in the B-site and the O-element is described as 1:3, even when the ratio of the element amounts is slightly shifted (for example, from 1.00:2.94 to 1.00:3.06), a metal oxide can be considered as a perovskite type metal oxide as long as the metal oxide has a perovskite structure as a main phase. From structure analysis, for example, by X-ray diffraction or electron beam diffraction, it can be determined that the metal oxide has a perovskite structure.

In the perovskite type metal oxide, elements A and B occupy specific positions in the form of ions in a unit lattice, which are called A-site and B-site. For example, in a cubic unit lattice, the element A is positioned at a vertex of the cube while the element B occupies the body-centered position of the cube. The element O occupies a face center position of the cube as an anion of oxygen. When the element A, the element B, and the element O are respectively shifted slightly on the coordinates from symmetric positions of the unit lattice, the unit lattice of the perovskite type structure is distorted to become a tetragonal, rhombohedral, or orthorhombic crystal system.

As a combination of valences that can be taken by an A-site ion and a B-site ion, there are given A⁺B⁵⁺O²⁻ ₃, A²⁺B⁴⁺O²⁻ ₃, A³⁺B³⁺O²⁻ ₃, and a solid solution obtained by a combination thereof. The valence may be an average valance of a plurality of ions positioned in the same site.

There is no particular limitation on the composition of the piezoelectric ceramic piece 1021 as long as the content of lead is smaller than 1,000 ppm (that is, lead-free). For example, piezoelectric ceramics having a composition containing barium titanate, barium calcium titanate, barium calcium zirconate titanate, bismuth sodium titanate, potassium sodium niobate, sodium barium titanate niobate, and bismuth ferrite, and piezoelectric ceramics containing those compositions as a main component can be used in the ultrasonic motor and the vibrator 1 of the present invention.

Of those, it is preferred that the piezoelectric ceramic piece 1021 contain a perovskite type metal oxide represented by one of the following general formulae (1) and (2). {M_(h)(Na_(j)Li_(k)K_(1-j-k))_(1-h)}_(1-m){(Ti_(1-u-v)Zr_(u)Hf_(v))_(h)(Nb_(1-w)Ta_(w))_(1-h)}O₃  (1) (where M represents at least one kind selected from the group consisting of (Bi_(0.5)K_(0.5)), (Bi_(0.5)Na_(0.5)), (Bi_(0.5)Li_(0.5)), Ba, Sr, and Ca, and 0.06<h≤0.3, 0≤j≤1, 0≤k≤0.3, 0≤j+k≤1, 0<u≤1, 0≤v≤0.75, 0≤w≤0.2, 0<u+v≤1, and −0.06≤m≤0.06.) (Ba_(1-s)Ca_(s))_(α)(Ti_(1-t)Zr_(t))O₃ (0.986≤α≤1.100, 0.02≤s≤0.30, and 0.020≤t≤0.095)  (2)

Further, it is preferred that the content of metal components other than the main component be 1 part by weight or less in terms of a metal with respect to 100 parts by weight of the metal oxide represented by the general formula.

In the general formulae (1) and (2), although the molar ratio between the element in the B-site and the O-element is described as 1:3, even when the ratio of the element amounts is slightly shifted (for example, from 1.00:2.94 to 1.00:3.06), the metal oxide falls within the scope of the present invention as long as the metal oxide has a perovskite type structure as a main phase. From the structure analysis, for example, by X-ray diffraction or electron beam diffraction, it can be determined that the metal oxide has a perovskite type structure.

(Main Component and Other Metal Components)

In the present invention, the term “main component” means that the piezoelectric ceramic piece 1021 contains 90 mass % or more of the perovskite type metal oxide represented by one of the general formulae (1) and (2) with respect to the total weight of the piezoelectric ceramic piece 1021. The piezoelectric ceramic piece 1021 contains more preferably 95 mass % or more, still more preferably 99 mass % or more of the perovskite type metal oxide.

In addition, it is preferred that the content of the metal components other than the main component be 1 part by weight or less in terms of a metal with respect to 100 parts by weight of the metal oxide represented by the general formula (1) or (2). The metal component refers to, for example, typical metals, transition metals, rare-earth elements, and semimetal elements such as Si, Ge, and Sb. The form of the metal component contained in the piezoelectric ceramic piece 1021 is not limited. For example, the metal component may be dissolved in solid in the A-site or the B-site of the perovskite type structure or may be contained in a grain boundary. The metal component may also be contained in the piezoelectric ceramic piece 1021 in the form of a metal, an ion, an oxide, a metal salt, a complex, or the like.

When one or more metal elements selected from Mn, Cu, Fe, and Bi is contained in the metal oxide represented by the general formula within a range of 1 part by weight or less in terms of a metal with respect to 100 parts by weight of the metal oxide, an insulation property and a mechanical quality factor of the piezoelectric ceramic piece 1021 are enhanced. Here, the mechanical quality factor refers to a factor representing elasticity loss caused by vibration of the piezoelectric element 102, and the magnitude of the mechanical quality factor is observed as steepness of a resonance curve in impedance measurement. That is, the mechanical quality factor is a constant representing the steepness of resonance of the piezoelectric element 102.

When the content of the metal component is more than 1 part by weight in terms of a metal with respect to 100 parts by weight of the metal oxide represented by the general formula, there is a risk in that the piezoelectric characteristics and insulation characteristics of the piezoelectric ceramic piece 1021 may be degraded.

There is no particular limitation on a method of measuring a composition of the piezoelectric ceramic piece 1021. As the method of measuring a composition, there are given X-ray fluorescence analysis, ICP emission spectroscopic analysis, and the like. The composition of the main component and the contents of the other metal components contained in the piezoelectric ceramic piece 1021 can be calculated by any of those methods.

(KNN-Based Piezoelectric Ceramics)

The general formula (1) represents a perovskite type metal oxide having piezoelectricity in which potassium sodium niobate (KNN) is used as a base material and Li, (Bi_(0.5)K_(0.5)), (Bi_(0.5)Na_(0.5)), (Bi_(0.5)Li_(0.5)), Ba, Sr, Ca, Ti, Zr, Hf, and Ta are subjected to site substitution in an amount of at most 30 atomic % or less in order to adjust characteristics.

The Young's modulus at room temperature (for example, 20° C.) of the piezoelectric ceramics containing the perovskite type metal oxide represented by the general formula (1) as a main component (hereinafter referred to as “KNN-based piezoelectric ceramics) falls within a range of from about 80 GPa to about 125 GPa. In the piezoelectric ceramics that can be used in the present invention, the Young's modulus of the KNN-based piezoelectric ceramics falls within a low range. Therefore, in order to obtain sufficient generation force during drive of the ultrasonic motor, it is preferred that a relationship: 2.00≤L_(top)/L_(btm)≤2.86 be satisfied. The more preferred range of L_(top)/L_(btm) is 2.40≤L_(top)/L_(btm)≤2.86. When the average values L_(top) and L_(btm) satisfy the above-mentioned relationship, the ultrasonic motor of the present invention using the KNN-based piezoelectric ceramics can transmit sufficient generation force while having appropriate friction between the vibrator 1 and the moving member 2.

The absolute value of the piezoelectric constant d₃₁ at room temperature of the KNN-based piezoelectric ceramics 1021 is large at, for example, 100 pm/V or more. Therefore, when the KNN-based piezoelectric ceramics is used in the ultrasonic motor of the present invention, a high rotation speed is obtained during motor drive.

In the general formula (1), “h” representing the molar ratio of M, which is a divalent or quasi divalent A-site metal, in the A-site falls within a range of 0.06≤h≤110.3. The abundance of Ti, Zr, and Hf, which are quadrivalent B-site metals, in the B-site is also introduced with the molar ratio h. With this, the charge balance (electrical neutrality) of the entire metal oxide is kept, and the insulation property of the piezoelectric ceramic piece 1021 can be ensured.

The A-site of the KNN-based piezoelectric ceramics is originally monovalent. However, when a part of the A-site is substituted with a divalent metal, a crystal structure changes, and the piezoelectric constant can be enhanced. However, when “h” is larger than 0.3, there is a risk in that a depolarization temperature may decrease to, for example, 100° C. or less.

The depolarization temperature (sometimes referred to as “T_(d)”) as used herein refers to temperature at which the piezoelectric constant decreases as compared to that before the temperature is raised at a time when, after an elapse of a sufficient time period from polarization treatment, the temperature is raised from room temperature to the temperature T_(d)(° C.) and lowered to room temperature again. Here, the temperature at which the piezoelectric constant becomes less than 90% of that before the temperature is raised is referred to as the depolarization temperature T_(d).

The B-site of the KNN-based piezoelectric ceramics is originally pentavalent. However, when a part of the B-site is substituted with quadrivalent Ti, Zr, or Hf, the transition temperature of a crystal structure changes, and the change in piezoelectric constant with respect to the environmental temperature can be suppressed. The effect of suppressing the change in piezoelectric constant with respect to the environmental temperature decreases in the order of Zr, Ti, and Hf. When “v” representing the details of Hf in the quadrivalent metals is larger than 0.75, the piezoelectric constant decreases, and there is a risk in that the rotation speed of the piezoelectric motor may decrease.

In the A-site of the general formula (1), the alkali metals excluding the above-mentioned “M” include Na, K, and Li. The total amount 1−h of the alkali metals in the A-site satisfies a relationship: 0.75≤1-h≤0.94. That is, a relationship: 0.06<h≤0.3 is satisfied. The bases of the alkali metals are Na and K, and the substitution amount k of Li is 0.3 or less. When Li is substituted within the above-mentioned range with respect to Na and K, there is an effect that the aspect ratio of a lattice constant of a perovskite structure is enhanced to increase the depolarization temperature.

In the general formula (1), “1−m” representing the molar ratio of constituent atoms in the A-site and the B-site of the perovskite structure falls within a range of 0.945≤1-m≤1.06. That is, a relationship: −0.065≤m≤0.06 is satisfied. Ideally, a stoichiometric ratio in which the number of constituent atoms in the A-site and the number of constituent atoms in the B-site have a ratio of 1:1, that is, a relationship: m=0 is preferred. However, in the actual step of manufacturing the KNN-based piezoelectric ceramics, “m” may change within a range of ±0.06. Within this range of “m”, the piezoelectric constant of the KNN-based piezoelectric ceramics does not significantly change.

A part of Nb in the B-site of the general formula (1) may be substituted with Ta, and the range of “w” representing the molar ratio of substitution is 0≤w≤0.2. When Ta is substituted within the range of the above-mentioned “w” with respect to Nb, the piezoelectric constant of the KNN-based piezoelectric ceramics is enhanced.

(BCTZ-Based Piezoelectric Ceramics)

The general formula (2) represents barium calcium zirconate titanate (BCTZ) obtained by substituting a part of Ba of barium titanate having a perovskite type structure with Ca and substituting a part of Ti thereof with Zr. When Ca and Zr are simultaneously substituted, the piezoelectric constant can be significantly enhanced without decreasing the depolarization temperature of the piezoelectric ceramic piece 1021. It is preferred that the crystal system of the perovskite type metal oxide represented by the general formula (2) have a tetragonal structure at room temperature because a satisfactory mechanical quality factor can be obtained.

The Young's modulus at room temperature (for example, 20° C.) of the BCTZ-based piezoelectric ceramic piece 1021 falls within a range of from about 80 GPa to about 125 GPa. In the piezoelectric ceramics that can be used in the present invention, the Young's modulus of the BCTZ-based piezoelectric ceramic piece 1021 falls within a high range, and hence the high generation force can be obtained during drive of the ultrasonic motor.

Meanwhile, the absolute value of the piezoelectric constant d₃₁ at room temperature of the BCTZ-based piezoelectric ceramic piece 1021 is large at, for example, about 90 pm/V or more. Therefore, when the BCTZ-based piezoelectric ceramic piece 1021 is used in the ultrasonic motor of the present invention, a high rotation speed is obtained even in a high load during motor drive.

In the general formula (2), “α” representing the ratio between the molar quantity of Ba and Ca in the A-site and the molar quantity of Ti and Zr in the B-site fall within a range of 0.9865≤α≤1.100. When “α” is smaller than 0.986, abnormal grain growth is liable to occur in crystal grains forming the piezoelectric ceramic piece 1021, and the mechanical strength of the piezoelectric ceramic piece 1021 is degraded. Meanwhile, when “α” is larger than 1.100, the temperature required for grain growth of the piezoelectric ceramic piece 1021 becomes too high, with the result that sintering cannot be performed in a general calcination furnace. Here, “sintering cannot be performed” refers to a state in which the density does not become a sufficient value and a great number of pores and defects are present in the piezoelectric ceramic piece 1021.

In the general formula (1), “s” representing the molar ratio of Ca in the A-site falls within a range of 0.02≤s≤0.30. When a part of Ba of perovskite type barium titanate is substituted with Ca within the above-mentioned range, the phase transition temperature of an orthorhombic crystal system and a tetragonal crystal system is shifted to a low temperature side, and hence stable piezoelectric vibration can be obtained within the drive temperature range of the ultrasonic motor and the vibrator 1. However, when “s” is larger than 0.30, the piezoelectric constant of the piezoelectric ceramic piece 1021 is not sufficient, and hence the rotation speed of the ultrasonic motor may become insufficient. Meanwhile, when “s” is smaller than 0.02, a sufficient mechanical quality factor is not obtained within the drive temperature range of the ultrasonic motor and the vibrator 1.

In the general formula (2), “t” representing the molar ratio of Zr in the B-site falls within a range of 0.020≤t≤0.095. When a part of the Ti-site is substituted with Zr within the above-mentioned range, the distortion of a tetragonal crystal system of the piezoelectric material is reduced, and hence c/a decreases to approach 1, with the result that large piezoelectric vibration can be obtained. The more preferred range of “t” is 0.040≤t≤0.085. When “t” is larger than 0.095, the depolarization temperature decreases, and there is a risk in that the drive of the ultrasonic motor may not be sufficient in a high temperature atmosphere, for example, at 50° C.

The common electrode 1022 is arranged on a surface of the annular piezoelectric ceramic piece 1021 on a side opposed to the vibrating plate 101, that is, a surface that is brought into contact with the vibrating plate 101 or a surface that is brought into contact with the above-mentioned adhesive layer. The common electrode 1022 is arranged in an annular manner similarly to the surface of the piezoelectric ceramic piece 1021. It is preferred that the common electrode 1022 be brought into conduction with a non-drive phase electrode 10232 (see FIG. 1B) among the plurality of electrodes 1023 so that a drive voltage can be applied to only a particular region of the plurality of electrodes 1023. For example, when wiring is arranged so as to be brought into contact with both the common electrode 1022 and the non-drive phase electrode 10232, both the common electrode 1022 and the non-drive phase electrode 10232 can be brought into conduction. Alternatively, wiring may be arranged so as to bring the common electrode 1022 and the non-drive phase electrode 10232 into conduction through intermediation of the vibrating plate 101 having conductivity.

Such wiring can be formed, for example, by applying a metal paste made of, for example, silver and drying or baking the metal paste.

As illustrated in FIG. 1B, the plurality of electrodes 1023 include two drive phase electrodes 10231, one or more non-drive phase electrodes 10232, and one or more detection phase electrodes 10233. It is preferred that the drive phase electrodes 10231, the non-drive phase electrode 10232, and the detection phase electrode 10233 not be brought into conduction with each other so that each electrode can have an independent potential during drive.

The detection phase electrode 10233 is arranged for the purpose of detecting a vibration state of the vibrator 1 and feeding back information on the vibration state to the outside, for example, a drive circuit. The piezoelectric ceramic piece 1021 in a region that is brought into contact with the detection phase electrode 10233 is subjected to polarization treatment. Therefore, when the ultrasonic motor is driven, a voltage corresponding to the magnitude of deformation (distortion) of the vibrator 1 is generated in a region of the detection phase electrode 10233 and output to the outside as a detection signal.

It is preferred that at least one non-drive phase electrode 10232 be brought into conduction with the common electrode 1022 because the non-drive phase electrode 10232 can be used as a ground electrode. An exemplary mode and procedure for obtaining conduction are as described above. When the drive phase electrode 10231, the non-drive phase electrode 10232 serving as a ground electrode, and the detection phase electrode 10233 are arranged on one surface (surface opposite to a surface on which the common electrode 1022 is arranged) of the annular piezoelectric element 102, the transmission of an electric signal (drive signal, detection signal) with respect to the outside of the ultrasonic motor is facilitated. For example, a drive signal and detection vibration can be transmitted through a flexible printed board.

When a flexible printed board is used for electrical connection of the ultrasonic motor and the drive circuit, the flexible printed board is arranged so as to be brought into contact with a part of each drive phase electrode 10231, the non-drive phase electrode 10232, and the detection phase electrode 10233 on one surface of the annular piezoelectric element 102 (surface on a side opposite to a surface which the common electrode 1022 faces). The flexible printed board has high dimension accuracy and can be positioned easily through use of a jig or the like. For connection of the flexible printed board, thermal pressure bonding can also be performed through use of an epoxy adhesive or the like. However, from the viewpoint of mass production, it is preferred that an anisotropic conductive paste (ACP) and an anisotropic conductive film (ACF) that have conductivity be subjected to thermal pressure bonding so that a conduction failure can be reduced and a process speed is increased. When thermal pressure bonding is used for connection of the flexible printed board, it is preferred to select a temperature lower than the depolarization temperature of the piezoelectric ceramic piece 1021.

The piezoelectric ceramic piece 1021 in a region that is in contact with the non-drive phase electrode 10232 may or may not have residual (remanent) polarization. When the piezoelectric ceramic piece 1021 in a region that is brought into contact with the non-drive phase electrode 10232 has residual polarization, it is preferred that the non-drive phase electrode 10232 and the common electrode 1022 be brought into conduction with each other.

As illustrated in FIG. 1B, each drive phase electrode 10231 includes six polarizing electrodes 102311 and a connecting electrode 102312 that electrically connects the six polarizing electrodes 102311.

FIG. 3 is a schematic view for illustrating a relationship between the circumferential length and the wavelength of a vibration wave in the annular piezoelectric element 102 to be used in the ultrasonic motor of the present invention. In FIG. 3, for convenience of description, the electrodes are not shown. The annular ring in FIG. 3 represents the piezoelectric element 102 and has substantially the same shape as that of the piezoelectric ceramic piece 1021. When an arbitrary position is designated on a surface of the annular ring, and the diameter of a circle that passes through the arbitrary position and shares its center with the annular shape of the piezoelectric element 102 is represented by 2R_(arb) (unit: mm), the circumferential length of the circle is 2πR_(arb). The circumferential length 2πR_(arb) is set to 7λ in the present invention. “λ” in the present invention refers to the wavelength at a time when a propagating wave of 7th order (wave number: 7) bending vibration is generated in the circumferential direction of the vibrator 1 forming the ultrasonic motor of the present invention. The value of λ varies depending on the arbitrary position designated above, but such parameter λ is assumed in order to design the shape and dimensions of the plurality of electrodes 1023. The circumferential length is hereinafter considered assuming the circle that passes through the arbitrary position on the surface of the piezoelectric element 102 even when there is no particular description.

FIG. 4A and FIG. 4B are each a schematic view for illustrating the arrangement of the polarizing electrodes 102311 in the annular piezoelectric element 102 to be used in the ultrasonic motor of the present invention and the polarity of the piezoelectric ceramic piece 1021 in each electrode region, when the annular piezoelectric element 102 is viewed from a side on which the plurality of electrodes are arranged. For convenience of description, in FIG. 4A and FIG. 4B, the connecting electrode 102312 is not shown. A combination of the polarities in FIG. 4A and FIG. 4B is an example and does not limit the present invention.

The piezoelectric ceramic piece 1021 in a region that is brought into contact with the drive phase electrode 10231 has residual polarization in a direction substantially perpendicular to the drive phase electrode 10231. A region having residual polarization may be a part or a whole of the piezoelectric ceramic piece 1021 in a region held between the polarizing electrodes 102311 and the common electrode 1022. From the viewpoint of enhancing the generation force during drive of the ultrasonic motor, it is preferred that the entire region held between the polarizing electrodes 102311 and the common electrode 1022 have residual polarization. In the present invention, the region having residual polarization is referred to as “polarized region”. The residual polarization refers to polarization that remains in the piezoelectric ceramic piece 1021 at a time when a voltage is not applied to the piezoelectric ceramic piece 1021. When the piezoelectric ceramic piece 1021 is subjected to polarization treatment, the direction of spontaneous polarization is aligned in a voltage application direction, and thus the piezoelectric ceramic piece 1021 has residual polarization. Whether or not the piezoelectric ceramic piece 1021 has residual polarization can be determined by applying voltage between the electrodes holding the piezoelectric element 102 and measuring an applied electric field E and a polarization amount P (P-E hysteresis curve).

Each drive phase electrode 10231 includes the six polarizing electrodes 102311, and correspondingly, there are six regions of the piezoelectric ceramic piece 1021 that are brought into contact with the polarizing electrodes 102311, that is, six polarized regions. The six polarized regions and the six polarizing electrodes 102311 are arranged along the circumference so as to sandwich unpolarized regions therebetween as illustrated in FIG. 4A and FIG. 4B. The polarities of the polarized regions are reversed alternately in order of the arrangement along the circumference. In FIG. 4A and FIG. 4B, symbols “+” and “−” written on an inner side of the polarizing electrodes 102311 represent directions of residual polarization, that is, polarities. In this specification, the symbol “+” is written in the electrode region to which a positive voltage is applied in the polarization treatment in the manufacturing step of the piezoelectric element 102. Therefore, when the piezoelectric constant d₃₃ is measured only in the “+” electrode region, a negative value is detected. Similarly, in the “−” electrode region, a positive piezoelectric constant d₃₃ is detected. Meanwhile, only in the electrode regions having the symbol “0” written in FIG. 4B or the unpolarized regions having no electrodes arranged in FIG. 4B, only the piezoelectric constant d₃₃ at room temperature of zero or an extremely small value, e.g., 5 pC/N or less is detected. In the piezoelectric element 102 illustrated in FIG. 4A and FIG. 4B, the piezoelectric ceramic piece 1021 includes a region having downward residual polarization and a region having upward residual polarization with respect to the drawing sheet. As a method of confirming that the polarity of residual polarization varies depending on the region, there are a method involving determining the variation in polarity based on the plus and minus of a value detected by measuring a piezoelectric constant and a method involving confirming that a shift direction from an original point of a coercive electric field in a P-E hysteresis curve is opposite.

Each polarized region and each polarizing electrode 102311 has substantially the same dimensions.

Specifically, it is preferred that the six polarizing electrodes 102311 (12 polarizing electrodes 102311 as a total of the two drive phase electrodes 10231) have an equal length in the circumferential direction. It is also preferred that each polarized region and each polarizing electrode 102311 have a difference of less than 2% in terms of a projection area.

More specifically, each polarizing electrode 102311 has a fan shape, and the length thereof in the circumferential direction is ideally λ/2 when the unpolarized regions are ignored. Actually, in order to prevent short-circuiting at a time when adjacent regions create polarized states having different polarities, the unpolarized regions are present between the respective polarizing electrodes 102311. In this case, it is ideal that the center of the unpolarized region in the circumferential direction be taken as a starting point, and a distance from the starting point to the center of the subsequent unpolarized region beyond the adjacent polarizing electrode 102311 be set to λ/2. However, an error of length of about less than 2% is allowed. From the viewpoint of enhancing drive force generated during drive of the ultrasonic motor, it is preferred that the volume of the unpolarized regions be as small as possible. The unpolarized regions sandwiched between the polarizing electrodes 102311 are brought into contact with the connecting electrode 102312.

The length of each drive phase electrode 10231 in the circumferential direction is ideally 3λ. Actually, there is a gap having no electrode in order to prevent short-circuiting with respect to the adjacent non-drive phase electrode 10232 or the detection phase electrode 10233, and hence the length is slightly smaller than 3λ. Actually, the length is set to be, for example, smaller than 3λ by from about 1% to about 2.5%.

The circumferential length of the circle that passes through an arbitrary position on the surface of the piezoelectric element 102 is 7λ, and hence a residual region of the circumferential length excluding the two drive phase electrodes 10231 is λ when the gap between the electrodes is ignored. The residual region is shared by one or more non-drive phase electrodes 10232 and one or more detection phase electrodes 10233. In this case, the two drive phase electrodes 10231 need to be separated from each other in the circumferential direction by two spacing regions having circumferential lengths of λ/4 and 3λ/4, respectively. The non-drive phase electrode 10232 and the detection phase electrode 10233 need to be arranged in two spacing regions. With this, phases of standing waves generated in regions of the two drive phase electrodes 10231, for example, the positions of nodes are shifted by λ/4, and the annular piezoelectric element 102 including the polarized regions having different polarities can form a bending vibration wave in the circumferential direction of the vibrator 1. This is because, when a voltage is applied simultaneously to each polarizing electrode 102311 through the connecting electrode 102312, one of the polarized regions expands and the other contracts in the circumferential direction due to the inverse piezoelectric effect.

When an alternating voltage having a frequency serving as a natural frequency of the vibrator 1 is applied to only a region sandwiched between one drive phase (phase A) electrode 10231 and the common electrode 1022 of the ultrasonic motor of the present invention, a standing wave having a wavelength λ is generated over the entire circumference along the circumferential direction on the surface of the vibrating plate 101. When an alternating voltage is similarly applied to only a region sandwiched between the other drive phase (phase B) electrode 10231 and the common electrode 1022, a similar standing wave is generated. The positions of nodes of the respective standing waves have a shift of λ/4 along the circumferential direction of the vibrating plate 101.

When the ultrasonic motor is driven, an alternating voltage having a frequency serving as a natural frequency of the vibrator 1 is applied to regions of the two drive phase (phase A and phase B) electrodes 10231 of the ultrasonic motor of the present invention so that the frequency is the same and a temporal phase difference becomes π/2. With this, due to the synthesis of the two standing waves, a 7th order propagating wave having the wavelength λ, which propagates in the circumferential direction, is generated in the vibrating plate 101.

The polarizing electrode 102311, the non-drive phase electrode 10232, the detection phase electrode 10233, and the connecting electrode 102312 are formed of a layer-like or film-like conductor having a resistance of less than 10Ω, preferably less than 1Ω. The resistance of the electrodes can be evaluated, for example, by measuring a resistance with a circuit tester (electric tester). The thickness of each electrode is from about 5 nm to about 20 μm. There is no particular limitation on the material for each electrode, and any material that is generally used in a piezoelectric element may be used.

As the material for the electrodes, there are given, for example, metals such as Ti, Pt, Ta, Ir, Sr, In, Sn, Au, Al, Fe, Cr, Ni, Pd, Ag, and Cu, and compounds thereof. The electrodes may be formed of one kind of the above-mentioned examples or laminations of two or more kinds thereof. The respective electrodes arranged in the piezoelectric element may be made of different materials.

Of those, as the electrode to be used in the present invention, an Ag paste or Ag baked electrode, an Au/Ti sputtered electrode, or the like is preferred because a resistance is low.

(Vibrating Plate)

As illustrated in FIG. 2, the second surface of the vibrating plate 101 that is brought into contact with the moving member 2 includes a plurality of groove regions 1012, each having a U-shaped cross-section, which extend radially. The “U-shaped cross-section” as used herein refers to a sectional shape having both wall surfaces substantially perpendicular to the second surface of the vibrating plate 101 and a bottom surface substantially horizontal thereto. The U-shaped cross-section broadly includes not only a so-called U-shape in which a bottom surface and each wall surface are smoothly connected to each other in a rounded manner, but also a shape similar to the so-called U-shape, which can be regarded as the “U-shaped cross-section”, such as a so-called rectangular shape in which a bottom surface and each wall surface are connected to each other so as to form a right angle, an intermediate shape thereof, or a shape slightly deformed from those shapes. FIG. 6B, FIG. 6C, and FIG. 6D are each an illustration of an exemplary sectional shape of a groove region having a U-shaped cross-section included in the present invention.

The second surface of the vibrating plate 101 includes the plurality of groove regions 1012 that are arranged radially, and hence a region between two adjacent groove regions forms a wall region 1011 that separates the two groove regions from each other. The plurality of groove regions 1012 extending radially are arranged in the circumferential direction, and hence the number of the wall regions 1011 formed therebetween is the same as that of the groove regions 1012. A top surface (ceiling surface) of the wall region 1011 corresponds to the second surface of the annular vibrating plate 101 and also serves as a reference surface for defining a depth of each groove region 1012. However, the wall region 1011 can be regarded as a convex region with respect to the groove region 1012 that is a concave region, and hence the wall region can also be referred to as “protrusion region”. That is, the moving member 2 can relatively move with respect to the vibrator 1, with which the moving member 2 is brought into pressure-contact, with drive force caused by friction with respect to the top surface of the protrusion region 1011. In the following, for convenience of description, the region 1011 between the groove regions 1012 is referred to as “protrusion region” instead of “wall region” in principle.

The groove regions 1012 of the present invention have a feature in that the center depth varies depending on each groove region 1012 (in FIG. 2, the center depth is shown as the same center depth). The “center depth” as used herein refers to a depth at a center position at a time when each groove region 1012 is viewed from the moving member 2 side. That is, the center depth refers to a depth of a groove measured from a top surface (second surface of the vibrating plate 101) of the protrusion region at a position corresponding to the center of each groove region both in the radial direction and the circumferential direction. In general, the bottom surface of the groove region 1012 is parallel as a whole to the second surface of the vibrating plate 101, is flat as a whole in the radial direction (direction in which the groove extends), and is flat as a whole in the circumferential direction (direction in which the grooves are arranged), or has a concave surface shape in which the center portion is flat and both side portions (vicinity of the wall surface) are raised. Therefore, the center depth means a depth of the deepest portion of each groove region. However, the foregoing varies depending on the bottom surface shape of each groove region, and hence the center depth does not necessarily always refer to the depth of the deepest portion. For example, the center depth may refer to a median value of a depth (for example, when the bottom surface is inclined in one direction). When the depth at the center position is a value that does not generally have a meaning as a representative value of a depth of the groove region (for example, a significant point), a value representing the depth of the groove region, which is a depth at another point close to the center position, is defined as a center depth. When a measurement position of a depth is fixed in all the groove regions, and the bottom surface of each groove region has the same shape, the significance of the center depth is the same in all the groove regions.

The protrusion regions (wall regions) 1011 and the groove regions 1012 are alternately arranged along the circumferential direction of the annular vibrating plate 101, and as described above, the number of the protrusion regions 1011 is the same as that of the groove regions 1012. It is assumed that the protrusion regions 1011 and the groove regions 1012 are each present in X portions. The number of the protrusion regions 1011 or the groove regions 1012 is determined so as to be substantially proportional to the outer diameter 2R of the vibrating plate 101, and so as to satisfy a relationship: ((2R/0.85)−5)≤X≤((2R/0.85)+15). Here, the units of 2R is mm, and X is a number. When X and 2R satisfy the above-mentioned relationship, the ultrasonic motor of the present invention can transmit sufficient drive force while having appropriate friction between the vibrator 1 and the moving member 2.

FIG. 5 is a graph for showing a relationship between the number of the groove regions 1012 (or the protrusion regions 1011) of the vibrating plate 101 and the outer diameter 2R of the vibrating plate 101. A colored region including the line segments of FIG. 5 falls within the scope of the present invention. It is not particularly necessary to provide an upper limit to the outer diameter 2R, but the description of the range in which the outer diameter 2R is more than 90 mm is not shown.

Meanwhile, the outer diameter 2R of the vibrating plate 101 is set to 57 mm or more, and hence a minimum value of the number X of the groove regions 1012 is 63. When the upper limit of the outer diameter 2R is 90 mm, a maximum value of the number X is 120. As another example, when the upper limit of the outer diameter 2R is 80 mm, the maximum value of the number X is 109.

When the number X of the groove regions 1012 is a natural number smaller than 2R/0.85−5, the deformation (distortion) of the protrusion regions 1011 that are brought into contact with the moving member 2 becomes insufficient, and as a result, the drive force generated by the vibrator 1 decreases. Meanwhile, when the number X is a natural number larger than 2R/0.85+15, the contact area with the moving member 2 for one protrusion region 1011 decreases. Therefore, when a weight body is used as an element on the moving member 2 side or large torque is applied to the moving member 2, the friction force between the moving member 2 and the protrusion regions 1011 becomes insufficient, and the drive force is not sufficiently transmitted, with the result that sliding may occur.

From the viewpoint of the generation force during motor drive and the prevention of sliding, the range of the number X is more preferably 85≤X≤100.

FIG. 6A to FIG. 6D are each a schematic view for illustrating a method of measuring lengths (unit: mm) in the circumferential direction (on the outer diameter side) of the protrusion region 1011 and the groove region 1012 of the annular vibrating plate 101 to be used in the ultrasonic motor of the present invention or the vibrator 1 of the present invention. When a boundary line between the protrusion region 1011 and the groove region 1012 extends accurately in the radial direction (that is, the groove region 1012 is formed in a fan shape), the ratio of the lengths thereof in the circumferential direction is the same even when the circumference is taken at any position on the surface of the vibrating plate 101. However, in general, the groove region 1012 does not have a fan shape and is formed into a shape in which the center line of the groove extends in the radial direction, and both wall surfaces extend in parallel to the center line (rectangular shape when viewed from the moving member 2 side). Thus, in a strict sense, the ratio of the lengths of the protrusion region 1011 and the groove region 1012 in the circumferential direction slightly varies depending on where the circumference is taken (radius of the virtual circle). In such case, the circumference is taken on the outer diameter side of the vibrating plate 101, and the radius of the virtual circle is set to R.

In the present invention, a ratio between an average value L_(top) of lengths of the protrusion regions 1011 in the circumferential direction on the outer diameter side and an average value L_(btm) of lengths of the groove regions 1012 in the circumferential direction on the outer diameter side is 2.00≤L_(top)/L_(btm)≤2.86. When the average values L_(top) and L_(btm) satisfy the above-mentioned relationship, the ultrasonic motor of the present invention can sufficiently transmit the drive force generated in the vibrator 1 while having appropriate friction force between the vibrator 1 and the moving member 2.

FIG. 6A is a schematic partial plan view of the vibrating plate 101 when viewed from a side of a surface (second surface) that is brought into contact with the moving member 2. It is assumed that one arbitrary protrusion region is selected from the protrusion regions (1011-1 to 1011-X) in X portions. The length (arc) of the selected protrusion region 1011-1 in the circumferential direction on the outer diameter side is represented by L_(top1). Lengths of the other protrusion regions 1011-2 to 1011-X in the circumferential direction on the outer diameter side are similarly determined, and an average of the lengths (L_(top1) to L_(topX)) in the X portions is determined to be the average value L_(top). An average is taken, and hence the lengths of the protrusion regions 1011 in the circumferential direction on the outer diameter side may be equal to or different from each other.

Similarly, one arbitrary groove region is selected from the groove regions (1012-1 to 1012-X) in the X portions. The length (arc) of the selected groove region 1012-1 in the circumferential direction on the outer diameter side is represented by L_(btm1). The lengths of the other groove regions 1012-2 to 1012-X in the circumferential direction on the outer diameter side are similarly determined, and an average of the lengths (L_(btm1) to L_(btmX)) in the X portions is determined to be the average value L_(btm). An average is taken, and hence the lengths of the groove regions 1012-1 to 1012-X in the circumferential direction on the outer diameter side may be equal to or different from each other.

FIG. 6B, FIG. 6C, and FIG. 6D are each a schematic developed view of a part of the vibrating plate 101 including the arbitrary protrusion region 1011-1 and the arbitrary groove region 1012-1 when viewed from the outer diameter side of the annular ring (position away from the annular ring in the radial direction). When the protrusion region 1011-1 and the groove region 1012-1 are formed into a rectangular shape or a substantially rectangular shape as illustrated in FIG. 6B, it is only necessary that the length of a ceiling side of the protrusion region (top surface on the outer diameter side) be set to the length L_(top1), and the length of a bottom side of the groove region (bottom surface on the outer diameter side) be set to the length L_(btm1).

When a wall surface common to the protrusion region 1011-1 and the groove region 1012-1 is perpendicular to the first surface of the vibrating plate 101, but the top surface of the protrusion region 1011-1 or the bottom surface of the groove region 1012-1 is not flat as illustrated in FIG. 6C, the lengths L_(top1) and L_(btm1) can be determined based on the distance between the wall surfaces on the outer diameter side. When the wall surface common to the protrusion region 1011-1 and the groove region 1012-1 is not perpendicular to the first surface of the vibrating plate 101 as illustrated in FIG. 6D, a perpendicular line to the first surface of the vibrating plate 101 is assumed at a position on the wall surface serving as an intermediate position between the center height of the protrusion region 1011-1 and the center depth of the groove region 1012-1, and this position may be used as a reference when measuring the lengths L_(top1) and L_(btm1).

When the ratio L_(top)/L_(btm) of the lengths of the protrusion region 1011 and the groove region 1012 in the circumferential direction on the outer diameter side is smaller than 2.00, the contact area of the protrusion regions 1011 in the X portions with respect to the moving member 2 decreases. Therefore, when a weight body is used as an element on the moving member 2 side or large torque (for example, 500 gf·cm or more) is applied to the moving member 2, the friction force between the moving member 2 and the protrusion regions 1011 becomes insufficient, and the drive force is not effectively transmitted to cause sliding, with the result that a drive speed may decrease. Meanwhile, when the ratio L_(top)/L_(btm) is larger than 2.86, the deformation (distortion) of the protrusion regions 1011 that are brought into contact with the moving member 2 becomes insufficient, with the result that the drive force generated by the vibrator 1 decreases, and hence the drive speed decreases.

The ratio L_(top)/L_(btm) is more preferably 2.00≤L_(top)/L_(btm)≤2.40.

In any of the cases of FIG. 6B, FIG. 6C, and FIG. 6D, further including cases not shown in those figures, from the viewpoint of increasing the contact with the moving member 2, it is preferred that the distances from the first surface of the vibrating plate 101, which serves as a starting point, to the maximum points of the protrusion regions 1011-1 to 1011-X be equal to each other within a range of tolerance of processing dimensions.

Center depths of the groove regions 1012 in the X portions are respectively represented by D₁ to D_(X) (unit: mm) in order of the circumferential direction of the vibrating plate 101. In the present invention, the center depths D₁ to D_(X) take five kinds or more of different values and change so as to follow a curve obtained by superimposing one or more sine waves on one another.

For example, in the case of suppressing 4th order, 5th order, 6th order, and 8th order (wave number along the annular ring is 4, 5, 6, and 8) propagating waves, which serve as the unnecessary vibration waves with respect to the 7th order propagating wave along the annular ring intended by the present invention, it is only necessary that the center depths D₁ to D_(X) are changed along the curve obtained by superimposing one or more and four or less sine waves on one another. A general formula of the curve obtained by superimposing sine waves on one another in that case is represented by the following expression (1). D=D _(ave) +Am ₄×sin(4×2×ω+θ₄)+Am ₅×sin(5×2×ω+θ₅)+Am ₆×sin(6×2×ω+θ₆)+Am ₈×sin(8×2×ω+θ₈)  Expression 1

In the expression (1), ω represents an angle indicating a center position of a groove of the annular vibrating plate 101 extending radially. θ represents an angle indicating a phase difference and is appropriately determined so as to satisfy conditions described later in the embodiment. D (unit: mm) represents a depth of an ideal groove at a center position of an arbitrary groove of the annular vibrating plate 101, and the center depths D₁ to D_(X) are set to D±0.1. The depth change of the respective values of the center depths D₁ to D_(X) is matched with D calculated by the expression (1). D_(ave) (unit: mm) represents a standard depth of the groove region 1012 that is set separately as an average value of the center depths D₁ to D_(X).

Am (unit: mm) is a real number to be an amplitude of each sine wave, and a suffix represents an order (wave number) of the unnecessary vibration waves intended to be reduced. Of Am₄, Am₅, Am₆, and Am₈, at least one takes a value other than 0. The number of amplitudes having values other than 0 is the number of sine waves to be superimposed on one another. There is no particular limitation on an upper limit thereof as long as the number of sine waves to be superimposed on one another is one or more. However, when five or more sine waves are superimposed on one another, the effect of reducing the unnecessary vibration waves is not substantially enhanced, and there is a risk in that the efficiency of motor drive may be degraded. Thus, it is preferred that the number of sine waves to be superimposed on one another be one or more and four or less. The more preferred number of sine waves to be superimposed on one another is two or more and four or less.

FIG. 7A, FIG. 7B, FIG. 7C and FIG. 7D, and FIG. 7E, FIG. 7F, FIG. 7G, and FIG. 7H are each a graph for schematically showing a distribution of a center depth of the groove regions of the vibrating plate of the ultrasonic motor according to the embodiment of the present invention. FIG. 7A and FIG. 7C, and FIG. 7E and FIG. 7G are each an example for showing a difference between the center depth and the standard depth D_(ave) of each groove region at a time when it is assumed that X is 90. A horizontal axis of each plot represents the order of 90 groove regions (hereinafter referred to as “groove number”). The 0th groove region does not actually exist, but is used for convenience on the plot so as to show the depth of the 90th groove region twice. The plots of a depth of each groove region in FIG. 7A and FIG. 7C, and FIG. 7E and FIG. 7G follow a curve obtained by superimposing four sine waves on one another in both cases.

FIG. 7B, FIG. 7D, and FIG. 7H are each a graph for schematically showing, as a graph plot, a relationship of the height of the protrusion region and the depth of the groove region in the case of application to the vibrating plate 101, with the center depth of each groove region shown in each of FIG. 7A, FIG. 7C, and FIG. 7G being the standard depth D_(ave) of 1.85 mm. In this example, the heights of the respective protrusion regions, with the first surface of the vibrating plate 101 being a starting point, are equal to each other. The horizontal axis of each plot represents positions of the 90 groove regions as angles when viewed from the center of the annular ring. The values on the horizontal axis are relative values, but in FIG. 7B, the center of the protrusion region sandwiched between the 89th groove region and the 90th (0th) groove region in FIG. 7A is set as a starting point.

Similarly, FIG. 7F is a graph for schematically showing, as a graph plot, a relationship of the height of the protrusion region and the depth of the groove region in the case of application to the vibrating plate 101, with the center depth of each groove region shown in FIG. 7E being the standard depth D_(ave) of 1.65 mm.

By setting the groove depth as shown in FIG. 7A, FIG. 7B, FIG. 7C, and FIG. 7D and FIG. 7E, FIG. 7F, FIG. 7G, and FIG. 7H, the generation of 4th order, 5th order, 6th order, and 8th order propagating waves being the unnecessary vibration waves are substantially suppressed with respect to the 7th order propagating wave. For example, when only the 4th order unnecessary vibration wave is focused on, the center depth of the groove region 1012 has local maximum regions (deep regions) in 8 portions and local minimum regions (shallow regions) in 8 portions at an equal interval (angle of π/4) with respect to the circumference as also represented by the second term (sin(4×2×ω+θ₄)) of the right side of the expression (1). The position of an antinode of each standing wave generated by the two drive phase electrodes 10231 is also shifted at an angle of π/4. Therefore, one standing wave vibrates in a portion having a low rigidity, and hence the resonant frequency is shifted to a low frequency side. The other standing wave vibrates in a portion having a high rigidity, and hence the resonant frequency is shifted to a high frequency side. The resonant frequencies of the standing waves are separated, with the result that the 4th order propagating wave (unnecessary vibration wave) is not generated. The same mechanism of suppression applies to the other order unnecessary vibration waves.

As a method of confirming that the center depth of the groove regions 1012 in the X portions in the vibrating plate 101 of the ultrasonic motor changes along the curve obtained by superimposing one or more sine waves on one another, there may be given the following method. First, coordinates and a depth of a center portion of each groove with respect to the circumferential length of the vibrating plate 101 on the outer diameter side are actually measured. The coordinates of the groove regions are taken on the horizontal axis, and the actually measured depth is taken on the vertical axis. Plots are complemented, and a curve in which a groove depth is present in all the coordinates is assumed. This curve is subjected to Fourier transformation to determine the presence and number of sine waves.

The center depth of the groove regions 1012 in the X portions changes so that the number of the groove regions which reach a local maximum and the number of the groove regions which reach a local minimum reaches 12 or more, respectively. The local maximum of the center depth indicates that the center depth of a certain groove region is larger than any center depth of the groove regions adjacent to the certain groove region on both sides. Similarly, the local minimum of the center depth indicates that the center depth of a certain groove region is smaller than any center depth of the groove regions adjacent to the certain groove region on both sides.

The ultrasonic motor and the vibrator 1 of the present invention use a 7th order bending vibration wave as a drive source of the moving member 2. The unnecessary vibration waves having significant adverse effects are 6th order and 8th order vibration waves having resonant frequencies close to that of the 7th order bending vibration wave. As represented by the fourth term of the right side of the expression (1), the 6th order unnecessary vibration wave having particularly large effects can be effectively suppressed by arranging 12 local maximum regions (deep regions) and 12 local minimum regions (shallow regions) in the groove regions 1012.

It is preferred that the number of the groove regions 1012 which reach a local maximum be matched with that of the groove regions 1012 which reach a local minimum. It is preferred that the number of the groove regions 1012 which reach a local maximum and the number of the groove regions 1012 which reach a local minimum be 16 or less, respectively. When an attempt is made to suppress the 8th unnecessary vibration wave, the number of the groove regions 1012 which reach a local maximum and the number of the groove regions 1012 which reach a local minimum may become 16, respectively. However, when the number becomes 17 or more, there is a risk in that the drive force generated by the ultrasonic motor and the vibrator 1 of the present invention may extremely decrease. It is more preferred that the number of the groove regions 1012 which reach a local maximum be from 12 to 16. With such configuration, the unnecessary vibration waves can be further effectively suppressed.

(Positional Relationship Between Local Maximum Region and Local Minimum Region of Center Depth)

In the groove regions 1012 in the X portions, the groove region in which the center depth reaches a local maximum and the groove region in which the center depth reaches a local minimum are arranged so as to sandwich one or more groove regions without being adjacent to each other. With this configuration, the rotation operation of the moving member 2 at a time when the ultrasonic motor and the vibrator 1 of the present invention are driven becomes more stable.

When the ultrasonic motor and the vibrator 1 of the present invention are driven, an elliptical motion occurs in a ceiling surface of each protrusion region 1011 to serve as power for rotating the moving member 2. The elliptical ratio of the elliptical motion depends on the center depth of the groove region. Therefore, when the center depth is small, the elliptical ratio becomes larger, and when the center depth is large, the elliptical ratio becomes smaller. The elliptical ratio differs greatly between the groove region in which the center depth reaches a local maximum and the groove region in which the center depth reaches a local minimum. Therefore, when those groove regions are adjacent to each other, the rotation operation of the moving member 2 does not become smoother, and the behavior of the rotation operation varies depending on the rotation direction.

It is preferred that, of the groove regions 1012 in the X portions which reach a local maximum, a number I of the groove regions positioned between the groove region having a largest center depth and the groove region having a second largest center depth satisfy a relationship: I≥X/18. With such configuration, the elliptical ratio becomes more uniform, and as a result, the rotation operation becomes even more stable, and the rotation speed increases.

It is preferred that, of the center depths D₁ to D_(X), a difference (change width) between the maximum value (groove having a largest center depth) and the minimum value (groove having a smallest center depth) be 5% or more and 25% or less with respect to the maximum thickness T_(dia) of the vibrating plate 101. By setting the change width of the center depths D₁ to D_(X) to within the above-mentioned range with respect to the maximum thickness T_(dia) of the vibrating plate 101, the suppression of the unnecessary vibration waves and the efficiency of the motor drive can be achieved. When the difference between the maximum value and the minimum value of the center depths D₁ to D_(X) is smaller than 5% with respect to the maximum thickness T_(dia), there is a risk in that the unnecessary vibration waves may not be sufficiently suppressed. Meanwhile, when the difference between the maximum value and the minimum value of the center depths D₁ to D_(X) is more than 25% with respect to the maximum thickness T_(dia), the transmission efficiency of vibration to the moving member 2 for each protrusion region 1011 varies, and hence there is a risk in that the drive efficiency of the motor may decrease.

FIG. 7A, FIG. 7B, FIG. 7C, and FIG. 7D and FIG. 7E, FIG. 7F, FIG. 7G, and FIG. 7H are each an example in which the center depth is designed so that the difference between the maximum value and the minimum value of the center depths D₁ to D_(X) is 5% or more and 25% or less with respect to the maximum thickness T_(dia), with the maximum thickness T_(dia) being set to 4 mm or more and 6 mm or less.

It is preferred that the standard depth D_(ave) of the center depths D₁ to D_(X) be 25% or more and 50% or less with respect to the maximum thickness T_(dia). By setting the standard depth D_(ave) to within the above-mentioned range with respect to the maximum thickness T_(dia) of the vibrating plate 101, the efficiency of the motor drive and the rotation speed can be achieved. When the standard depth D_(ave) is smaller than 25% with respect to the maximum thickness T_(dia), the deformation amount during drive of the vibrating plate 101 decreases, and there is a risk in that the rotation speed of the motor may decrease. Meanwhile, when the standard depth D_(ave) is more than 50% with respect to the maximum thickness T_(dia), there is a risk in that the drive efficiency of the motor may decrease.

It is preferred that, of the groove regions in which the center depth reaches a local maximum, 8 or more groove regions have the center depth of 1.15 times or more and 1.30 times or less of the standard depth D_(ave). With such configuration, a load is uniformly applied to each groove, and hence the rotation speed increases particularly in a high load.

When the number X is an even number, it is preferred that, of the center depths D₁ to D_(X), the depth change of the former half D₁ to D_(X/2) (rows of center depths of the respective groove regions) be matched with that of the latter half D_(X/2+1) to D_(X). The groove region 1012 serving as a starting point may be arbitrarily selected. Therefore, when X is equal to, for example, 90, it is preferred that a relationship: D_(n)=D_(n+45) holds with respect to any n. In this case, the depth change of 45 continuous groove regions 1012 and the depth change of 45 remaining continuous groove regions 1012 are matched in the same circumferential direction. With such configuration, the suppression of the unnecessary vibration waves is further enhanced, and the symmetric property of the rotation motion of the moving member 2 becomes satisfactory.

Of the groove regions 1012 in the X portions, the center depth of the groove region 1012 closest to the detection phase electrode 10233 is represented by D_(sen)(unit: mm). The term “sen” as used herein relates to a natural number of 1 or more and X or less. The groove region 1012 closest to the detection phase electrode 10233 is determined with the center of the detection phase electrode 10233 being a reference point. The center depths of two groove regions 1012 adjacent to the groove region 1012 closest to the detection phase electrode 10233 are represented by D_(sen−1) and D_(sen+1). In this case, it is preferred that |D_(sen+1)−D_(sen−1)|/D_(sen) be 5% or less. When the relationship of the center depths of the three groove regions is set to within the above-mentioned range, the center depths of both the adjacent groove regions 1012 having the detection phase electrode 10233 as a center become closer to each other. As a result, the amplitude of the vibrator 1 in the vicinity of the detection phase electrode 10233 during drive of the ultrasonic motor becomes substantially the same irrespective of whether the drive is clockwise drive or counterclockwise drive, and hence the drive control of the ultrasonic motor by the drive circuit becomes easier.

The ultrasonic motor using a 7th order bending vibration wave is described above as an example, but the present invention is also applicable to a case using another order bending vibration wave. For example, unnecessary vibration waves other than the 6th order unnecessary vibration wave may be suppressed in an ultrasonic motor using a 6th order bending vibration wave. Similarly, the present invention can be applied to ultrasonic motors using any bending vibration waves such as an 8th order bending vibration wave and a 11th order bending vibration wave.

(Drive Control System)

Next, the drive control system of the present invention is described. FIG. 8 is a schematic view for illustrating the drive control system according to an embodiment of the present invention.

The drive control system of the present invention has a feature of including at least the ultrasonic motor of the present invention and a drive circuit electrically connected to the ultrasonic motor. The drive circuit includes a signal generation unit configured to generate an electric signal for generating a 7th order bending vibration wave in the ultrasonic motor of the present invention to cause rotation drive.

The drive circuit simultaneously applies alternating voltages having the same frequency and a temporal phase difference of π/2 to each drive phase electrode 10231 (phase A and phase B) of the ultrasonic motor. As a result, standing waves generated in the phase A and the phase B are synthesized to generate a propagating wave of a 7th order bending vibration wave (wavelength: λ), which propagates in the circumferential direction, on the second surface of the vibrating plate 101.

In this case, each point on the protrusion regions 1011 in the X portions of the vibrating plate 101 undergoes elliptical motion. Therefore, the moving member 2 rotates due to the friction force in the circumferential direction from the vibrating plate 101. When the 7th order bending propagating wave is generated, the detection phase electrode 10233 generates a detection signal in accordance with the amplitude of vibration of the piezoelectric ceramic piece 1021 in the regions brought into contact with the detection phase electrode 10233 and outputs the detection signal to the drive circuit through wiring. The drive circuit compares the detection signal with the phase of the drive signal input to the drive phase electrode 10231, to thereby grasp a shift from a resonant state. By determining again the frequency of the drive signal input to the drive phase electrode 10231 based on the above-mentioned information, the feedback control of the ultrasonic motor can be performed.

(Optical Apparatus)

Next, the optical apparatus of the present invention is described. The optical apparatus of the present invention includes at least the drive control system of the present invention and an optical element dynamically connected to the ultrasonic motor included in the drive control system.

The phrase “dynamic connection” as used herein refers to a state in which elements are directly in contact with each other or a state in which the elements are in contact with each other through intermediation of a third element so that force generated by a coordinate change, a volume change, and a shape change of one element is transmitted to the other element.

FIG. 9A and FIG. 9B are each a sectional view of main parts of an interchangeable lens barrel for a single-lens reflex camera as an example of an optical apparatus according to an exemplary embodiment of the present invention. FIG. 10 is an exploded perspective view of the interchangeable lens barrel for the single-lens reflex camera as the example of the optical apparatus according to the exemplary embodiment of the present invention. A fixed barrel 712, a linear guide barrel 713, and a front lens unit barrel 714 holding a front lens group 701 are fixed to a detachable mount 711 for a camera. Those components are fixed elements of the interchangeable lens barrel.

A linear guide groove 713 a in an optical axis direction for a focus lens 702 is formed on the linear guide barrel 713. Cam rollers 717 a and 717 b protruding outward in a radial direction are fixed to a rear lens unit barrel 716 holding the focus lens 702 via axial screws 718, and the cam roller 717 a is fitted in the linear guide groove 713 a.

A cam ring 715 is fitted on the inner periphery of the linear guide barrel 713 in a rotatable manner. Relative movement between the linear guide barrel 713 and the cam ring 715 in the optical axis direction is restricted due to a roller 719 fixed to the cam ring 715 being fitted in an annular groove 713 b of the linear guide barrel 713. A cam groove 715 a for the focus lens 702 is formed on the cam ring 715, and the above-mentioned cam roller 717 b is simultaneously fitted in the cam groove 715 a.

On the outer peripheral side of the fixed barrel 712, there is arranged a rotation transmission ring 720 held by a ball race 727 in a rotatable manner at a predetermined position with respect to the fixed barrel 712. The rotation transmission ring 720 has shafts 720 f extending radially from the rotation transmission ring 720, and rollers 722 are held by the shafts 720 f in a rotatable manner. A large diameter region 722 a of the roller 722 makes contact with a mount side end surface 724 b of a manual focus ring 724. In addition, a small diameter part 722 b of the roller 722 makes contact with a joining member 729. Six rollers 722 are arranged on the outer periphery of the rotation transmission ring 720 at uniform intervals, and each roller is provided in the relationship as described above.

A low friction sheet (washer member) 733 is arranged on an inner diameter region of the manual focus ring 724, and this low friction sheet is sandwiched between a mount side end surface 712 a of the fixed barrel 712 and a front side end surface 724 a of the manual focus ring 724. In addition, an outer diameter surface of the low friction sheet 733 is formed into a ring shape so as to be circumferentially fitted on an inner diameter region 724 c of the manual focus ring 724. Further, the inner diameter region 724 c of the manual focus ring 724 is circumferentially fitted on an outer diameter region 712 b of the fixed barrel 712. The low friction sheet 733 has a role of reducing friction in a rotation ring mechanism in which the manual focus ring 724 rotates relatively to the fixed barrel 712 about the optical axis.

Note that, the large diameter region 722 a of the roller 722 makes contact with the mount side end surface 724 b of the manual focus ring under a state in which a pressure is applied by a pressing force of a wave washer 726 pressing an ultrasonic motor 725 to the front of the lens. In addition, similarly, the small diameter region 722 b of the roller 722 makes contact with the joining member 729 under a state in which an appropriate pressure is applied by a pressing force of the wave washer 726 pressing the ultrasonic motor 725 to the front of the lens. Movement of the wave washer 726 in the mount direction is restricted by a washer 732 connected to the fixed barrel 712 by bayonet joint. A spring force (biasing force) generated by the wave washer 726 is transmitted to the ultrasonic motor 725, and further to the roller 722, to be a force for the manual focus ring 724 to press the mount side end surface 712 a of the fixed barrel 712. In other words, the manual focus ring 724 is integrated under a state in which the manual focus ring 724 is pressed to the mount side end surface 712 a of the fixed barrel 712 via the low friction sheet 733.

Therefore, when a drive circuit having a signal generation unit built therein (not shown) drives the ultrasonic motor 725 to rotate with respect to the fixed barrel 712, the rollers 722 rotate about the shafts 720 f so that the joining member 729 is brought into contact by friction with the small diameter regions 722 b of the rollers 722. As a result of the rotation of the rollers 722 about the shafts 720 f, the rotation transmission ring 720 rotates about the optical axis (automatic focus operation).

In addition, when a manual operation input unit (not shown) gives a rotation force about the optical axis to the manual focus ring 724, the components are operated as follows.

Specifically, the rollers 722 rotate about the shafts 720 f by friction force because the mount side end surface 724 b of the manual focus ring 724 is brought into pressure-contact with the large diameter regions 722 a of the rollers 722. When the large diameter regions 722 a of the rollers 722 rotate about the shafts 720 f, the rotation transmission ring 720 rotates about the optical axis. In this case, the ultrasonic motor 725 does not rotate because of a friction retaining force between a moving member 725 c and a vibrator 725 b (manual focus operation).

Two focus keys 728 are mounted to the rotation transmission ring 720 at opposing positions, and the focus key 728 is fitted to a notch portion 715 b formed in the tip of the cam ring 715. Therefore, when the automatic focus operation or the manual focus operation is performed so that the rotation transmission ring 720 is rotated about the optical axis, the rotation force is transmitted to the cam ring 715 via the focus key 728. When the cam ring 715 is rotated about the optical axis, the rear lens unit barrel 716 whose rotation is restricted by the cam roller 717 a and the linear guide groove 713 a is moved forward and backward along the cam groove 715 a of the cam ring 715 by the cam roller 717 b. Thus, the focus lens 702 is driven, and the focus operation is performed. That is, the position of the focus lens 702, which is an optical element, is changed by the focus lens 702 being dynamically connected to the ultrasonic motor 725.

In this case, the interchangeable lens barrel for the single-lens reflex camera is described above as the optical apparatus of the present invention, but the present invention can be applied to many kinds of optical apparatus including the ultrasonic motor, regardless of a type of the camera, including a compact camera, an electronic still camera, and the like.

EXAMPLES

Next, the vibrator, the ultrasonic motor, the drive control system, and the optical apparatus of the present invention are specifically described by means of Examples, but the present invention is not limited to the following Examples. The Examples are described with reference to the drawings with use of the reference symbols in the drawings.

(Manufacturing Example of Annular Piezoelectric Ceramic Piece)

An annular piezoelectric ceramic piece containing lead in a content of less than 1,000 ppm and having a Young's modulus at room temperature of 80 GPa or more and 125 GPa or less was manufactured in the following manner. The Young's modulus was measured through use of a test piece cut out from a piezoelectric element.

(Manufacturing Example of KNN-Based Piezoelectric Ceramics)

With intent to add Cu to [{Ba_(0.75)(Bi_(0.5)Na_(0.5))_(0.25)}_(0.08)(Na_(0.49)Li_(0.02)K_(0.49))_(0.92)]_(1.00){(Ti_(0.20)Zr_(0.75)Hf_(0.05))_(0.08)(Nb_(0.90)Ta_(0.10))_(0.92)}O₃ corresponding to the composition of h of 0.08, j of 0.49, k of 0.02, u of 0.75, v of 0.05, w of 0.10, and m of 0 in the general formula (1), with the metal M being Ba_(0.75) (Bi_(0.5)Na_(0.5))_(0.25), corresponding raw material powders were weighed as follows.

Barium carbonate, bismuth oxide, sodium carbonate, lithium carbonate, potassium carbonate, titanium oxide, zirconium oxide, hafnium oxide, niobium pentoxide, and tantalum pentoxide, each being commercially available with a purity of 99.9% or more, serving as raw material powders, were weighed so that Ba, Bi, Na, Li, K, Ti, Zr, Hf, Nb, and Ta satisfied the composition of [{Ba_(0.75)(Bi_(0.5)Na_(0.5))_(0.25)}_(0.08)(Na_(0.49)Li_(0.02)K_(0.49))_(0.92)]_(1.00){(Ti_(0.20)Zr_(0.75)Hf_(0.05))_(0.08)(Nb_(0.90)Ta_(0.10))_(0.92)}O₃. The composition was able to be sintered at low temperature, and hence the loading ratio was set as intended without considering the volatilization of alkali metal components during the sintering step. Manganese dioxide was weighed so that the content of Mn was 0.25 part by weight with respect to 100 parts by weight of the composition of [{Ba_(0.75)(Bi_(0.5)Na_(0.5))_(0.25)}_(0.08)(Na_(0.49)Li_(0.02)K_(0.49))_(0.92)]_(1.00){(Ti_(0.20)Zr_(0.75)Hf_(0.05))_(0.08)(Nb_(0.90)Ta_(0.10))_(0.92)}O₃.

Those weighed powders were mixed by dry blending for 24 hours through use of a ball mill to provide mixed powder. In order to granulate the obtained mixed powder, 3 parts by weight of a PVA binder with respect to the mixed powder was caused to adhere to the surface of the mixed powder through use of a spray dryer, to thereby provide granulated powder.

Next, the obtained granulated powder was supplied to a mold, and a molding pressure of 200 MPa was applied to the granulated powder through use of a press molding machine to produce a disc-shaped molding. The dimensions of the mold used for the disc-shaped molding had a margin of 2 mm, 2 mm, and 0.5 mm with respect to the outer diameter, the inner diameter, and the thickness of the intended disc-shaped piezoelectric ceramics, respectively.

The obtained molding was placed in an electric furnace and held at a highest temperature of 1,000° C. for 10 hours, to thereby sinter the molding in an atmospheric atmosphere over a total of 48 hours. Next, the sintered body was ground into an annular shape having a desired outer diameter, inner diameter, and thickness to provide an annular piezoelectric ceramic piece.

Piezoelectric ceramic pieces, which were manufactured so as to have an outer diameter within a range of from 54 mm to 90 mm, an inner diameter within a range of from 38 mm to 84 mm, and a thickness within a range of from 0.3 mm to 1.0 mm, were able to have equivalent piezoelectric characteristics. The vibrator and the ultrasonic motor of the present invention can be manufactured through use of a piezoelectric ceramic piece having any dimensions within the above-mentioned ranges. However, for convenience of description, an annular piezoelectric ceramic piece having an outer diameter of 77.0 mm, an inner diameter of 67.1 mm, and a thickness of 0.5 mm is described as a typical example.

The average circle equivalent diameter and the relative density of crystal grains forming the manufactured piezoelectric ceramic piece were evaluated, and a piezoelectric ceramic piece having an average circle equivalent diameter of from 0.5 μm to 10.0 μm and a relative density of 95% or more was used for manufacturing a piezoelectric element in the next step. For calculation of the average circle equivalent diameter, a polarization microscope and a scanning electron microscope were used. The relative density was measured by the Archimedes' method and evaluated with respect to a theoretical density calculated from a lattice constant of the piezoelectric ceramic piece and an atomic weight of a constituent element of the piezoelectric ceramic piece.

It was found from the X-ray diffraction measurement of an annular surface that any of the piezoelectric ceramic pieces manufactured by the above-mentioned method had a perovskite structure.

The composition of the piezoelectric ceramic piece was evaluated by ICP emission spectroscopic analysis. As a result, the content of lead of any of the piezoelectric ceramic pieces manufactured by the above-mentioned method was less than 5 ppm. Through the combination of the results of ICP emission spectroscopic analysis and X-ray diffraction measurement, it was found that the composition of the piezoelectric ceramic piece contained, as a main component, a perovskite type metal oxide which can be represented by the composition of [{Ba_(0.75)(Bi_(0.5)Na_(0.5))_(0.25)}_(0.08)(Na_(0.49)Li_(0.02)K_(0.49))_(0.92)]_(1.00){(Ti_(0.20)Zr_(0.75)Hf_(0.05))_(0.08)(Nb_(0.90)Ta_(0.10))_(0.92)}O₃ and contained 0.25 part by weight of Mn with respect to 100 parts by weight of the main component.

(Manufacturing Example of BCTZ-Based Piezoelectric Ceramics)

With intent to add Mn and Bi to (Ba_(0.84)Ca_(0.16))_(1.006)(Ti_(0.94)Zr_(0.06))O₃ corresponding to the composition of s of 0.16, t of 0.06, and a of 1.006 in the general formula (2), corresponding raw material powders were weighed as follows.

Barium titanate, calcium titanate, and calcium zirconate each having an average particle diameter of 300 nm or less and a perovskite type structure, serving as raw material powders, were weighed so that Ba, Ca, Ti, and Zr satisfied the composition of (Ba_(0.84)Ca_(0.16))_(1.006)(Ti_(0.94)Zr_(0.06))O₃. In order to adjust “α” representing the molar ratio of the A-site and the B-site, barium carbonate and titanium oxide were used. Trimanganese tetroxide was weighed so that the content of Mn was 0.18 part by weight in terms of a metal with respect to 100 parts by weight of the composition of (Ba_(0.84)Ca_(0.16))_(1.006)(Ti_(0.94)Zr_(0.06))O₃. Similarly, bismuth oxide was weighed so that the content of Bi was 0.26 part by weight in terms of a metal.

Those weighed powders were mixed by dry blending for 24 hours through use of a ball mill to provide mixed powder. In order to granulate the obtained mixed powder, 3 parts by weight of a PVA binder with respect to the mixed powder was caused to adhere to the surface of the mixed powder through use of a spray dryer, to thereby provide granulated powder.

Next, the obtained granulated powder was supplied to a mold, and a molding pressure of 200 MPa was applied to the granulated powder through use of a press molding machine to produce a disc-shaped molding. The dimensions of the mold used for the disc-shaped molding had a margin of 2 mm, 2 mm, and 0.5 mm with respect to the outer diameter, the inner diameter, and the thickness of intended disc-shaped piezoelectric ceramics, respectively.

The obtained molding was placed in an electric furnace and held at a highest temperature of 1,380° C. for 5 hours, to thereby sinter the molding in an atmospheric atmosphere over a total of 24 hours. Next, the sintered body was ground into an annular shape having a desired outer diameter, inner diameter, and thickness to provide an annular piezoelectric ceramic piece.

Piezoelectric ceramic pieces, which were manufactured so as to have an outer diameter within a range of from 54 mm to 90 mm, an inner diameter within a range of from 38 mm to 84 mm, and a thickness within a range of from 0.3 mm to 1.0 mm, were able to have equivalent piezoelectric characteristics. The vibrator and the ultrasonic motor of the present invention can be manufactured through use of a piezoelectric ceramic piece having any dimensions within the above-mentioned ranges. However, for convenience of description, an annular piezoelectric ceramic piece having an outer diameter of 77.0 mm, an inner diameter of 67.1 mm, and a thickness of 0.5 mm is described as a typical example.

The average circle equivalent diameter and the relative density of crystal grains forming the manufactured piezoelectric ceramic piece were evaluated, and a piezoelectric ceramic piece having an average circle equivalent diameter of from 0.7 μm to 3.0 μm and a relative density of 95% or more was used for manufacturing a piezoelectric element in the next step. For calculation of the average circle equivalent diameter, a polarization microscope and a scanning electron microscope were used. The relative density was measured by the Archimedes' method and evaluated with respect to a theoretical density calculated from a lattice constant of the piezoelectric ceramic piece and an atomic weight of a constituent element of the piezoelectric ceramic piece.

It was found from the X-ray diffraction measurement of an annular surface that any of the piezoelectric ceramic pieces manufactured by the above-mentioned method had a tetragonal perovskite structure.

The composition of the piezoelectric ceramic piece was evaluated by ICP emission spectroscopic analysis. As a result, the content of lead of any of the piezoelectric ceramic pieces manufactured by the above-mentioned method was less than 1 ppm. Through the combination of the results of ICP emission spectroscopic analysis and X-ray diffraction measurement, it was found that the composition of the piezoelectric ceramic piece contained, as a main component, a perovskite type metal oxide which can be represented by the composition of (Ba_(0.84)Ca_(0.16))_(1.006)(Ti_(0.94)Zr_(0.06))O₃ and contained 0.18 part by weight of Mn and 0.26 part by weight of Bi with respect to 100 parts by weight of the main component.

Manufacturing Example 1 of Vibrating Plate

FIG. 11A and FIG. 11B are each a schematic step view for illustrating an example of a method of manufacturing an annular vibrating plate to be used in the ultrasonic motor and the vibrator of the present invention.

In order to manufacture a vibrating plate to be used in the present invention, an annular metal plate 101 a as illustrated in FIG. 11A was prepared. The metal plate 101 a is formed of magnetic stainless steel SUS420J2 of JIS. SUS420J2 is martensite stainless steel that is an alloy containing 70 mass % or more of steel and 12 mass % to 14 mass % of chromium.

The outer diameter, inner diameter, and maximum thickness of the metal plate 101 a were set to intended values of the outer diameter 2R, the inner diameter 2R_(in), and the maximum thickness T_(dia) of the vibrating plate 101 illustrated in FIG. 11B. A vibrating plate applicable to the vibrator and the ultrasonic motor of the present invention was able to be manufactured with the metal plate 101 a having an outer diameter (2R) within a range of from 56 mm to 90 mm, an inner diameter within a range of from 40 mm to 84 mm, and a thickness within a range of from 4 mm to 6 mm. In this manufacturing example, for convenience of description, the metal plate 101 a having the outer diameter 2R of 77 mm, the inner diameter 2R_(in) of 67.1 mm, and the maximum thickness T_(dia) of 5.0 mm is described as a typical example.

Next, 90 (X=90) groove regions 1012 were mechanically formed in a radial manner by grinding one surface (second surface) of the annular metal plate 101 a (grooving step). The metal plate 101 a after grooving was subjected to barrel treatment, lapping, and electroless nickel plating, to thereby provide the vibrating plate 101 to be used in the vibrator 1 of the present invention.

The groove region 1012 of the vibrating plate 101 was formed into a rectangular parallelepiped shape having a width of 0.895 mm when viewed from the second surface side. Therefore, the protrusion region 1011 was formed into a fan shape having a width enlarged on the annular outer diameter side. As a result, the average value L_(top) of the length of the protrusion region 1011 in the circumferential direction on the outer diameter side and the average value L_(btm) of the length of the groove region 1012 in the circumferential direction on the outer diameter side had a relationship: L_(top)/L_(btm)=2.00.

Center depths D₁ to D₉₀ of the 90 groove regions 1012 of the vibrating plate 101 were set to depths as shown in FIG. 7A. That is, the center depths D₁ to D₉₀ change so as to follow a curve obtained by superimposing four sine waves on one another. As is understood from FIG. 7A and FIG. 7B corresponding to FIG. 7A, the numbers of local maximum regions and local minimum regions of the change were 12, respectively. The local maximum regions and the local minimum regions of the change were not adjacent to each other. The maximum absolute value of the center depths D₁ to D₉₀ was 2.216 mm, and the minimum absolute value thereof was 1.493 mm. Therefore, a difference therebetween was 0.722 mm, which was 14.45% with respect to the maximum thickness T_(dia) (5.0 mm) of the vibrating plate 101. The average of the absolute values of the center depths D₁ to D₉₀ was 1.85 mm, which was 37.0% with respect to the maximum thickness T_(dia) (5.0 mm) of the vibrating plate 101.

Of the groove regions 1012 in which the center depth reaches a local maximum, the groove region 1012 having a largest center depth was D₃₀=D₇₅=2.216 mm, and the groove region 1012 having a second largest center depth was D₈=D₆₃=2.164 mm. The number I of the groove regions 1012 positioned between the groove region 1012 having a largest center depth and the groove region 1012 having a second largest center depth was 11 at a minimum.

Of the groove regions in which the center depth reaches a local maximum, 6 groove regions have the center depths D₁₈, D₃₀, D₄₀, D₆₃, D₇₅, and D₈₅ of 1.15 times or more and 1.30 times or less of the standard depth D_(ave).

The depth change of the center depths D₁ to D₄₅ and the depth change of the center depths D₄₆ to D₉₀ were as shown in Table 1. In Table 1, a suffix of D_(X) is shown in a large size so that the suffix can be easily recognized visually. As is understood from Table 1, of the center depths D₁ to D₉₀, the change in the center depths D₁ to D_(90/2) was matched with the change in the center depths D_(90/2+1) to D₉₀. With such configuration, the unnecessary vibration waves other than the 7th order vibration wave can be further suppressed.

TABLE 1 Symbol of center Symbol of center depth of groove Groove depth depth of groove Groove depth region [mm] region [mm] D30 2.216 D75 2.216 D18 2.164 D63 2.164 D40 2.160 D85 2.160 D19 2.117 D64 2.117 D1 2.115 D46 2.115 D29 2.108 D74 2.108 D31 2.099 D76 2.099 D2 2.083 D47 2.083 D39 2.046 D84 2.046 D41 2.045 D86 2.045 D8 2.028 D53 2.028 D9 2.027 D54 2.027 D10 2.006 D55 2.006 D11 1.991 D56 1.991 D17 1.975 D62 1.975 D7 1.927 D52 1.927 D20 1.924 D65 1.924 D12 1.918 D57 1.918 D23 1.906 D68 1.906 D45 1.898 D90 1.898 D32 1.891 D77 1.891 D24 1.881 D69 1.881 D38 1.834 D83 1.834 D3 1.832 D48 1.832 D28 1.823 D73 1.823 D22 1.818 D67 1.818 D21 1.792 D66 1.792 D42 1.772 D87 1.772 D33 1.747 D78 1.747 D13 1.741 D58 1.741 D6 1.723 D51 1.723 D25 1.708 D70 1.708 D34 1.702 D79 1.702 D37 1.691 D82 1.691 D35 1.689 D80 1.689 D16 1.676 D61 1.676 D36 1.666 D81 1.666 D44 1.635 D89 1.635 D4 1.591 D49 1.591 D43 1.575 D88 1.575 D27 1.574 D72 1.574 D5 1.556 D50 1.556 D14 1.543 D59 1.543 D26 1.543 D71 1.543 D15 1.493 D60 1.493

Manufacturing Example 2 of Vibrating Plate

A vibrating plate V2 was manufactured through use of the same raw materials and manufacturing method as those of the vibrating plate V1. The vibrating plate V2 was manufactured so as to satisfy L_(top)/L_(btm)=2.40.

The center depths D₁ to D₉₀ of the 90 groove regions 1012 of the vibrating plate 101 were set to those shown in FIG. 7D. That is, the center depths D₁ to D₉₀ change so as to follow a curve obtained by superimposing four sine waves on one another. As is understood from FIG. 7D and FIG. 7C corresponding to FIG. 7D, the numbers of local maximum regions and local minimum regions of the change were 12, respectively. The local maximum regions and the local minimum regions of the change were not adjacent to each other. The maximum absolute value of the center depths D₁ to D₉₀ was 2.202 mm, and the minimum absolute value thereof was 1.498 mm. Therefore, a difference therebetween was 0.703 mm, which was 14.1% with respect to the maximum thickness T_(dia) (5.0 mm) of the vibrating plate 101. The average of the absolute values of the center depths D₁ to D₉₀ was 1.85 mm, which was 37.0% with respect to the maximum thickness T_(dia) (5.0 mm) of the vibrating plate 101.

Of the groove regions 1012 in which the center depth reaches a local maximum, the groove region 1012 having a largest center depth was D₃₀=D₇₅=2.202 mm, and the groove region 1012 having a second largest center depth was D₈=D₆₃=2.169 mm. The number I of the groove regions 1012 positioned between the groove region 1012 having a largest center depth and the groove region 1012 having a second largest center depth was 9 at minimum.

Of the groove regions 1012 in which the center depth reaches a local maximum, there were 8 groove regions 1012 in which the center depth is 1.15 times or more and 1.30 times or less of the standard depth D_(ave) in the regions of the depths D₁, D₁₈, D₃₀, D₄₀, D₄₆, D₆₃, D₇₅, and D₈₅.

The change in the center depths D₁ to D₄₅ and the change in the center depths D₄₆ to D₉₀ were as shown in Table 2. In Table 2, a suffix of D_(X) is shown in a large size so that the suffix can be easily recognized visually. As is understood from Table 2, of the center depths D₁ to D₉₀, the change in the center depths D₁ to D_(90/2) was matched with the change in the center depths D_(90/2+1) to D₉₀. With such configuration, the unnecessary vibration waves other than the 7th order vibration wave can be further suppressed.

TABLE 2 Symbol of center Symbol of center depth of groove Groove depth depth of groove Groove depth region [mm] region [mm] D30 2.202 D75 2.202 D40 2.169 D85 2.169 D18 2.140 D63 2.140 D29 2.135 D74 2.135 D1 2.131 D46 2.131 D39 2.094 D84 2.094 D31 2.070 D76 2.070 D19 2.053 D64 2.053 D2 2.037 D47 2.037 D11 2.017 D56 2.017 D10 2.014 D55 2.014 D17 2.006 D62 2.006 D9 2.002 D54 2.002 D41 1.999 D86 1.999 D8 1.998 D53 1.998 D45 1.962 D90 1.962 D23 1.955 D68 1.955 D7 1.933 D52 1.933 D12 1.923 D57 1.923 D22 1.888 D67 1.888 D32 1.885 D77 1.885 D20 1.883 D65 1.883 D28 1.868 D73 1.868 D38 1.867 D83 1.867 D24 1.865 D69 1.865 D21 1.816 D66 1.816 D3 1.774 D48 1.774 D33 1.770 D78 1.770 D6 1.766 D51 1.766 D16 1.722 D61 1.722 D34 1.721 D79 1.721 D13 1.715 D58 1.715 D42 1.713 D87 1.713 D44 1.686 D89 1.686 D37 1.679 D82 1.679 D35 1.674 D80 1.674 D25 1.647 D70 1.647 D36 1.631 D81 1.631 D5 1.593 D50 1.593 D27 1.585 D72 1.585 D4 1.577 D49 1.577 D43 1.564 D88 1.564 D14 1.518 D59 1.518 D15 1.506 D60 1.506 D26 1.498 D71 1.498

Manufacturing Example 3 of Vibrating Plate

A vibrating plate V3 was manufactured through use of the same raw materials and manufacturing method as those of the vibrating plate V1. The vibrating plate V3 was manufactured so as to satisfy T_(dia)=6.0 mm, D_(ave)=1.65 mm and L_(top)/L_(btm)=2.40.

The center depths D₁ to D₉₀ of the 90 groove regions 1012 of the vibrating plate 101 were set to those shown in FIG. 7F. That is, the center depths D₁ to D₉₀ change so as to follow a curve obtained by superimposing four sine waves on one another. As is understood from FIG. 7F and FIG. 7E corresponding to FIG. 7F, the numbers of local maximum regions and local minimum regions of the change were 12, respectively. The local maximum regions and the local minimum regions of the change were not adjacent to each other. The maximum absolute value of the center depths D₁ to D₉₀ was 2.016 mm, and the minimum absolute value thereof was 1.292 mm. Therefore, a difference therebetween was 0.724 mm, which was 12.1% with respect to the maximum thickness T_(dia) (6.0 mm) of the vibrating plate 101. The average of the absolute values of the center depths D₁ to D₉₀ was 1.65 mm, which was 27.5% with respect to the maximum thickness T_(dia) (6.0 mm) of the vibrating plate 101.

Of the groove regions 1012 in which the center depth reaches a local maximum, the groove region 1012 having a largest center depth was D₃₀=D₇₅=2.016 mm, and the groove region 1012 having a second largest center depth was D₈=D₆₃=1.963 mm. The number I of the groove regions 1012 positioned between the groove region 1012 having a largest center depth and the groove region 1012 having a second largest center depth was 11 at minimum.

Of the groove regions 1012 in which the center depth reaches a local maximum, there were 8 groove regions 1012 in which the center depth is 1.15 times or more and 1.30 times or less of the standard depth D_(ave) in the regions of the depths D₁, D₁₈, D₃₀, D₄₀, D₄₆, D₆₃, D₇₅, and D₈₅.

The change in the center depths D₁ to D₄₅ and the change in the center depths D₄₆ to D₉₀ were as shown in Table 3. In Table 3, a suffix of D_(X) is shown in a large size so that the suffix can be easily recognized visually. As is understood from Table 3, of the center depths D₁ to D₉₀, the change in the center depths D₁ to D_(90/2) was matched with the change in the center depths D_(90/2+1) to D₉₀. With such configuration, the unnecessary vibration waves other than the 7th order vibration wave can be further suppressed.

TABLE 3 Symbol of center Symbol of center depth of groove Groove depth depth of groove Groove depth region [mm] region [mm] D30 2.016 D75 2.016 D18 1.963 D63 1.963 D40 1.960 D85 1.960 D19 1.920 D64 1.920 D1 1.913 D46 1.913 D29 1.903 D74 1.903 D31 1.903 D76 1.903 D2 1.886 D47 1.886 D41 1.850 D86 1.850 D39 1.843 D84 1.843 D8 1.828 D53 1.828 D9 1.828 D54 1.828 D10 1.806 D55 1.806 D11 1.791 D56 1.791 D17 1.770 D62 1.770 D20 1.728 D65 1.728 D7 1.724 D52 1.724 D12 1.720 D57 1.720 D23 1.705 D68 1.705 D32 1.695 D77 1.695 D45 1.693 D90 1.693 D24 1.683 D69 1.683 D3 1.638 D48 1.638 D38 1.630 D83 1.630 D28 1.617 D73 1.617 D22 1.617 D67 1.617 D21 1.593 D66 1.593 D42 1.578 D87 1.578 D33 1.548 D78 1.548 D13 1.545 D58 1.545 D6 1.519 D51 1.519 D25 1.512 D70 1.512 D34 1.502 D79 1.502 D37 1.489 D82 1.489 D35 1.489 D80 1.489 D16 1.471 D61 1.471 D36 1.466 D81 1.466 D44 1.432 D89 1.432 D4 1.394 D49 1.394 D43 1.377 D88 1.377 D27 1.371 D72 1.371 D5 1.354 D50 1.354 D14 1.346 D59 1.346 D26 1.344 D71 1.344 D15 1.292 D60 1.292

Manufacturing Example 4 of Vibrating Plate

A vibrating plate V4 was manufactured through use of the same raw materials and manufacturing method as those of the vibrating plate V1. The vibrating plate V4 was manufactured so as to satisfy L_(top)/L_(btm)=2.86.

The center depths D₁ to D₉₀ of the 90 groove regions 1012 of the vibrating plate 101 were set to those shown in FIG. 7H. That is, the center depths D₁ to D₉₀ change so as to follow a curve obtained by superimposing four sine waves on one another. As is understood from FIG. 7H and FIG. 7G corresponding to FIG. 7H, the numbers of local maximum regions and local minimum regions of the change were 12, respectively. The local maximum regions and the local minimum regions of the change were not adjacent to each other. The maximum absolute value of the center depths D₁ to D₉₀ was 2.180 mm, and the minimum absolute value thereof was 1.494 mm. Therefore, a difference therebetween was 0.687 mm, which was 13.7% with respect to the maximum thickness T_(dia) (5.0 mm) of the vibrating plate 101. The average of the absolute values of the center depths D₁ to D₉₀ was 1.85 mm, which was 37.0% with respect to the maximum thickness T_(dia) (5.0 mm) of the vibrating plate 101.

Of the groove regions 1012 in which the center depth reaches a local maximum, the groove region 1012 having a largest center depth was D₃₀=D₇₅=2.180 mm, and the groove region 1012 having a second largest center depth was D₄₀=D₈₅=2.177 mm. The number I of the groove regions 1012 positioned between the groove region 1012 having a largest center depth and the groove region 1012 having a second largest center depth was 9 at minimum.

Of the groove regions 1012 in which the center depth reaches a local maximum, there were 6 groove regions 1012 in which the center depth is 1.15 times or more and 1.30 times or less of the standard depth D_(ave) in the regions of the depths D₁₈, D₃₀, D₄₀, D₆₃, D₇₅, and D₈₅.

The change in the center depths D₁ to D₄₅ and the change in the center depths D₄₆ to D₉₀ were as shown in Table 4. In Table 4, a suffix of D_(X) is shown in a large size so that the suffix can be easily recognized visually. As is understood from Table 4, of the center depths D₁ to D₉₀, the change in the center depths D₁ to D_(90/2) was matched with the change in the center depths D_(90/2+1) to D₉₀. With such configuration, the unnecessary vibration waves other than the 7th order vibration wave can be further suppressed.

TABLE 4 Symbol of center Symbol of center depth of groove Groove depth depth of groove Groove depth region [mm] region [mm] D30 2.180 D75 2.180 D40 2.177 D85 2.177 D18 2.133 D63 2.133 D29 2.132 D74 2.132 D1 2.127 D46 2.127 D39 2.116 D84 2.116 D31 2.053 D76 2.053 D11 2.041 D56 2.041 D19 2.031 D64 2.031 D10 2.031 D55 2.031 D17 2.021 D62 2.021 D2 2.017 D47 2.017 D9 1.993 D54 1.993 D41 1.985 D86 1.985 D45 1.979 D90 1.979 D8 1.973 D53 1.973 D23 1.965 D68 1.965 D12 1.930 D57 1.930 D7 1.918 D52 1.918 D22 1.911 D67 1.911 D32 1.893 D77 1.893 D28 1.885 D73 1.885 D38 1.877 D83 1.877 D20 1.870 D65 1.870 D24 1.852 D69 1.852 D21 1.827 D66 1.827 D33 1.795 D78 1.795 D6 1.776 D51 1.776 D3 1.761 D48 1.761 D16 1.740 D61 1.740 D34 1.738 D79 1.738 D44 1.703 D89 1.703 D13 1.699 D58 1.699 D42 1.694 D87 1.694 D37 1.665 D82 1.665 D35 1.665 D80 1.665 D25 1.627 D70 1.627 D5 1.615 D50 1.615 D36 1.607 D81 1.607 D27 1.601 D72 1.601 D4 1.587 D49 1.587 D43 1.562 D88 1.562 D15 1.506 D60 1.506 D14 1.498 D59 1.498 D26 1.494 D71 1.494

Manufacturing Example of Vibrating Plate for Comparison

For comparison with the present invention, a vibrating plate V5 was manufactured through use of the same raw materials and manufacturing method as those of the vibrating plate V1. The center depths D₁ to D₉₀ of the groove regions in the 90 portions of the vibrating plate V5 were all set to 1.85 mm, and the vibrating plate V5 was manufactured so as to satisfy a relationship: L_(top)/L_(btm)=1.24.

For comparison with the present invention, a vibrating plate V6 was manufactured through use of the same raw materials and manufacturing method as those of the vibrating plate V1. The center depths D₁ to D₉₀ of the groove regions in the 90 portions of the vibrating plate V6 were all set to 1.85 mm, and the vibrating plate V6 was manufactured so as to satisfy a relationship: L_(top)/L_(btm)=4.40.

Here, the features of the vibrating plates V1, V2, V3, V4, V5, and V6 are summarized in Table 5.

TABLE 5 Difference between maximum Outer Inner value and diameter diameter Groove Local Local minimum L_(top) L_(btm) 2R 2R_(in) number X L_(top)/ maximum minimum T_(da) value of D₁ − [mm] [mm] [mm] [mm] [portions] L_(btm) [pieces] [pieces] [mm] D_(x) [mm] Vibrating 1.793 0.895 77.0 67.1 90 2.00 12 12 5 0.722 plate V1 Vibrating 1.897 0.791 77.0 67.1 90 2.40 12 12 5 0.703 plate V2 Vibrating 1.897 0.791 77.0 67.1 90 2.40 12 12 6 0.724 plate V3 Vibrating 1.991 0.697 77.0 67.1 90 2.86 12 12 5 0.687 plate V4 Vibrating 1.488 1.200 77.0 67.1 90 1.24 12 12 5 0.000 plate V5 Vibrating 1.488 0.338 77.0 67.1 90 4.40 12 12 5 0.000 plate V6 Number I of groove Difference regions between between maximum largest value and groove minimum Average region and value of D₁ − value of D₁ second 100 × D_(x) with to D_(x) with largest |D_(sen+1) − D_(sen−1)|/ respect to D_(ave) respect to Number of groove D_(sen) T_(da) [mm] T_(da) [%] sine waves region [%] Vibrating 14.4% 1.85 37.0% 4 11 0.05% plate V1 Vibrating 14.1% 1.85 37.0% 4 9 0.31% plate V2 Vibrating 12.1% 1.65 27.5% 4 11 0.01% plate V3 Vibrating 13.7% 1.85 37.0% 4 9 0.02% plate V4 Vibrating 0.0% 1.85 0.0% 0 0 0.00% plate V5 Vibrating 0.0% 1.85 0.0% 0 0 0.00% plate V6

Manufacturing Example and Comparative Example of Vibrator

FIG. 12A, FIG. 12B, FIG. 12C, FIG. 12D, and FIG. 12E are each a schematic step view for illustrating an example of a method of manufacturing the vibrator and the ultrasonic motor of the present invention.

The KNN-based piezoelectric ceramics and the BCTZ-based piezoelectric ceramics described in the above-mentioned manufacturing examples, and the vibrating plates V1, V2, V3, V4, V5, and V6 were combined to manufacture 12 vibrators. The manufacturing examples thereof are shown in Table 6.

TABLE 6 Vibrating Piezoelectric plate ceramics Manufacturing Example 1 V1 KNN Example 1 Manufacturing Example 2 V2 KNN Example 2 Manufacturing Example 3 V3 KNN Example 3 Manufacturing Example 4 V4 KNN Example 4 Manufacturing Example 5 V1 BCTZ Example 5 Manufacturing Example 6 V2 BCTZ Example 6 Manufacturing Example 7 V3 BCTZ Example 7 Manufacturing Example 8 V4 BCTZ Example 8 Manufacturing Comparative V5 KNN Example 9 Example 1 Manufacturing Comparative V6 KNN Example 10 Example 2 Manufacturing Comparative V5 BCTZ Example 11 Example 3 Manufacturing Comparative V6 BCTZ Example 12 Example 4

First, the annular piezoelectric ceramic piece 1021 was subjected to screen printing of a silver paste, to thereby form the common electrode 1022 on one surface as illustrated in FIG. 12C and the polarizing electrodes 102311 in 12 portions, the non-drive phase electrodes 10232 in 3 portions, and the detection phase electrode 10233 in 1 portion on the other surface as illustrated in FIG. 12B. In this case, the distance between the respective adjacent electrodes illustrated in FIG. 12B was set to 0.5 mm.

Next, polarization treatment was performed between the common electrode 1022, and the polarizing electrodes 102311, the non-drive phase electrodes 10232, and the detection phase electrode 10233 in air through use of a DC power source so that the expansion and contraction polarity of the piezoelectric element became as illustrated in FIG. 4A. The voltage was set to a value at which an electric field of 1.0 kV/mm was applied, and the temperature and the voltage application time were set to 100° C. and 60 minutes, respectively. The voltage was applied during a decrease in temperature until the temperature reached 40° C.

Next, as illustrated in FIG. 12D, in order to connect the polarizing electrodes 102311, the connecting electrode 102312 was formed through use of a silver paste, and both kinds of the electrodes were combined to form the drive phase electrodes 10231 in 2 portions, to thereby provide the piezoelectric element 102. The silver paste was dried at temperature sufficiently lower than the depolarization temperature of the piezoelectric ceramic piece 1021. A resistance of the drive phase electrode 10231 was measured with a circuit tester (electric tester). One side of the circuit tester was brought into contact with the surface of a portion of the polarizing electrodes 102311 closest to the detection phase electrode 10233, and the other side thereof was brought into contact with the surface of a portion of the polarizing electrodes 102311 farthest from the detection phase electrode 10233 in the circumferential direction of the annular shape in the drive phase electrode 10231. As a result, the resistance of the drive phase electrode 10231 was 0.6Ω.

In this stage, as a sampling inspection of the piezoelectric element 102, a test piece was cut out and various characteristics of the piezoelectric ceramic piece 1021 were evaluated. Specifically, in the piezoelectric element 102, a rectangular strip having, for example, a length of 10 mm, a width of 2.5 mm, and a thickness of 0.5 mm was cut out from a region of one polarizing electrode 102311. The strip was measured by the resonance-antiresonance method at room temperature (20° C.), to thereby obtain the piezoelectric constant d₃₁, the mechanical quality factor Q_(m), and the Young's modulus Y₁₁. The results are shown in Table 7.

TABLE 7 Piezoelectric Mechanical constant quality factor Young's modulus Kind d₃₁ [pm/V] Q_(m) [—] Y₁₁ [10⁹ Pa] KNN 100 100 95 BCTZ 95 1,200 120 (Note) Measurement results at room temperature (20° C.)

Next, as illustrated in FIG. 12E, a flexible printed board 3 was pressure-bonded onto a region extending across the drive phase electrodes 10231 in 2 portions, the non-drive phase electrodes 10232 in 2 portions, and the detection phase electrode 10233 of the piezoelectric element 102 in a room temperature process through use of a moisture-curable epoxy resin adhesive. The flexible printed board 3 is an element to be arranged for the purpose of supplying electricity to the electrode group and taking out a detection signal, and includes electric wiring 301, an insulating base film 302, and a connector region (not shown) to be connected to an external drive circuit.

Next, as illustrated in FIG. 1A, the piezoelectric element 102 was pressure-bonded onto the first surface of the vibrating plate 101 (any of V1, V2, V3, V4, V5, and V6) in a room temperature process through use of a moisture-curable epoxy resin adhesive, and the vibrating plate 101 and the non-drive phase electrodes 10232 in 3 portions were connected to each other through short-circuited wiring (not shown) formed of a silver paste, to thereby manufacture the vibrator 1 of the present invention or a vibrator for comparison. The silver paste was dried at temperature sufficiently lower than the depolarization temperature of the piezoelectric ceramic piece 1021. The Young's modulus at room temperature of the epoxy adhesive after curing was measured in accordance with JIS K6911 to be about 2.5 GPa.

In the vibrator 1 using the vibrating plate V1, pressure bonding was performed so that the 40th groove region of FIG. 7A was arranged so as to be closest to the detection phase electrode 10233. In this case, the relationship of the center depths of the 39th, 40th, and 41st groove regions was |D₄₁−D₃₉|/D₄₀=0.05%.

In the vibrator 1 using the vibrating plate V2, pressure bonding was performed so that the 21st groove region of FIG. 7C was arranged so as to be closest to the detection phase electrode 10233. In this case, the relationship of the center depths of the 20th, 21st, and 22nd groove regions was |D₂₂−D₂₀|/D₂₁=0.31%.

In the vibrator 1 using the vibrating plate V3, pressure bonding was performed so that the 30th groove region of FIG. 7E was arranged so as to be closest to the detection phase electrode 10233. In this case, the relationship of the center depths of the 29th, 30th, and 31st groove regions was |D₃₁−D₂₉|/D₃₀=0.01%.

In the vibrator 1 using the vibrating plate V4, pressure bonding was performed so that the 36th groove region of FIG. 7G was arranged so as to be closest to the detection phase electrode 10233. In this case, the relationship of the center depths of the 35th, 36th, and 37th groove regions was |D₃₇−D₃₅|/D₃₆=0.02%.

(Evaluation of Unnecessary Vibration Wave at Resonant Frequency of Vibrator)

The resonant frequency of the vibrator 1 of the present invention obtained in each of the above-mentioned manufacturing examples was measured, to thereby determine the number of bending vibration waves to be generated, and a difference from the vibrator for comparison was evaluated.

The resonant frequency was measured for each drive phase electrode (phase A and phase B) 10231. First, in order to apply an alternating voltage to only the phase A electrode, the phase B electrode and the detection phase electrode 10233 were short-circuited to the non-drive phase electrode 10232 through use of the connector region of the flexible printed board 3, and the short-circuited region was connected through wiring to a ground side of an external power source for evaluation. An alternating voltage having a variable frequency and an amplitude of 1 V was applied to the phase A electrode, to thereby measure an impedance at room temperature. The frequency was changed from a high frequency side, for example, 50 kHz to a low frequency side, for example, 1 kHz. Then, the phase A electrode and the detection phase electrode 10233 were short-circuited to the non-drive phase electrode 10232, and an alternating voltage was applied to only the phase B electrode. Then, frequency dependence of an impedance was similarly measured.

In the vibrators for comparison (Manufacturing Examples 9, 10, 11, and 12) using the vibrating plate V5 or V6 in which the center depth of the groove regions did not change, the 6th order, 7th order, and 8th order resonant frequencies were matched between the impedance curves measured respectively in the phase A and the phase B. That is, it was found that, when the phase A standing wave and the phase B standing wave are combined, the 6th order and 8th order unnecessary propagating waves other than the desired 7th order propagating wave are also generated.

Meanwhile, in the vibrators 1 of the present invention using the vibrating plates V1, V2, V3, and V4 (Manufacturing Examples 1 to 8) in which the center depth of the groove regions changed in accordance with the present invention, the desired 7th order resonant frequency was matched between the impedance curves measured respectively in the phase A and the phase B, but the 6th order and 8th order unnecessary resonant frequencies indicated different peak positions. That is, it was found that, when the phase A standing wave and the phase B standing wave are combined, the generation of the 6th order and 8th order unnecessary propagating waves is suppressed with respect to the generation of the desired 7th order propagating wave.

Manufacturing Example of Moving Member

The moving member 2 was manufactured so as to be used in the ultrasonic motor of the present invention and the ultrasonic motor for comparison.

The shape of the moving member 2 was set to an annular shape, and the outer diameter, inner diameter, and thickness thereof were set to 77.0 mm, 67.1 mm, and 5 mm, respectively. An aluminum metal was used as a material for the moving member 2 and shaped by block machining. Then, the surface was subjected to alumite treatment.

Manufacturing Example and Comparative Example of Ultrasonic Motor

As illustrated in FIG. 1A and FIG. 2, the moving member 2 adjusted to the size of the vibrating plate 101 was brought into pressure-contact with the second surface of the vibrator 1 of the present invention, to thereby manufacture the ultrasonic motor of the present invention. Similarly, the ultrasonic motor for comparison was manufactured.

Manufacturing Example and Comparative Example of Drive Control System

The drive phase electrodes 10231, the non-drive phase electrodes 10232 short-circuited to the common electrode 1022, and the detection phase electrode 10233 in the ultrasonic motor of the present invention were electrically connected to an external drive circuit through use of the connector region of the flexible printed board 3, to thereby manufacture the drive control system of the present invention having the configuration as illustrated in FIG. 8. The external drive circuit includes a control unit configured to drive the ultrasonic motor and a signal generation unit configured to output an alternating voltage for generating a 7th order bending vibration wave in response to an instruction of the control unit.

Similarly, a drive control system for comparison was manufactured.

(Evaluation of Maximum Rotation Speed of Ultrasonic Motor)

The maximum rotation speed of the ultrasonic motor was evaluated through use of the drive control systems of the present invention (drive control systems 1 to 8) and the drive control systems for comparison (drive control systems 9 and 12).

Specifically, two kinds of loads: 150 gf·cm and 700 gf·cm were set by applying a load to the moving member 2. Alternating voltages were applied to the phases A and B of the drive circuit so as to obtain an amplitude of 70 V, the same frequency, and a temporal phase difference of π/2. Then, the maximum rotation speed of the ultrasonic motor at a time when the frequency was swept from 40 kHz to 25 kHz was evaluated. The results are shown in Table 8. In the 7th column of Table 8, a reduction in maximum rotation number at a time when the load was changed from 150 gf·cm to 700 gf·cm is shown in terms of a percent (reduction ratio (%) of the maximum rotation number).

TABLE 8 Maximum Maximum rotation rotation speed at speed at Reduction 150 700 in maximum Ultrasonic L_(top)/ gf · cm gf · cm rotation Abnormal motor Vibrator L_(btm) [rpm] [rpm] number (%) noise Drive control Ultrasonic Example 1 2.00 79 62 22% Absent system 1 motor 1 Drive control Ultrasonic Example 2 2.40 82 66 20% Absent system 2 motor 2 Drive control Ultrasonic Example 3 2.40 80 63 21% Absent system 3 motor 3 Drive control Ultrasonic Example 4 2.86 78 60 23% Absent system 4 motor 4 Drive control Ultrasonic Example 5 2.00 90 70 22% Absent system 5 motor 5 Drive control Ultrasonic Example 6 2.40 92 74 20% Absent system 6 motor 6 Drive control Ultrasonic Example 7 2.40 90 71 21% Absent system 7 motor 7 Drive control Ultrasonic Example 8 2.86 90 69 23% Absent system 8 motor 8 Drive control Ultrasonic Comparative 1.24 68 20 71% Present system 9 motor 9 Example 1 Drive control Ultrasonic Comparative 4.40 60 40 33% Present system 10 motor 10 Example 2 Drive control Ultrasonic Comparative 1.24 75 25 67% Present system 11 motor 11 Example 3 Drive control Ultrasonic Comparative 4.40 74 45 39% Present system 12 motor 12 Example 4

The drive control systems using the vibrators and the ultrasonic motors of the Examples exhibited maximum rotation speeds of the ultrasonic motor higher than those of the drive control systems for comparison in both the cases of 150 gf·cm and 700 gf·cm. In Comparative Examples 1 to 4 using the vibrating plates V5 and V6, the reduction ratio of a rotation speed at a time when the load was changed from 150 gf·cm to 700 gf·cm was large, and the reduction ratio was large particularly in Comparative Examples 1 and 3.

In the Examples, equivalent rotation drive was observed in any rotation direction, and abnormal noise was not generated during rotation drive. After the test, the moving member 2 was removed, and the shapes of the protrusion regions 1011 of the vibrating plate 101 were checked. However, no loss caused by abrasion was observed.

Meanwhile, in the drive control systems for comparison, abnormal noise was generated during rotation drive.

Manufacturing Example of Optical Apparatus

The optical apparatus illustrated in FIG. 9A and FIG. 9B, and FIG. 10 was manufactured through use of the drive control system of the present invention, and an autofocus operation in accordance with the application of an alternating voltage was checked. Even in a high load, the autofocus speed was sufficiently higher than that of the optical apparatus of Comparative Examples.

According to the present invention, there can be provided an ultrasonic motor configured to rotate a moving member with a 7th order bending vibration wave, in which a desired drive speed is exhibited with sufficient torque even when lead-free piezoelectric ceramics having high environmental safety is used, a drive control system and an optical apparatus that use the ultrasonic motor, and a vibrator to be used in the ultrasonic motor.

While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.

This application claims the benefit of Japanese Patent Application No. 2015-231902, filed Nov. 27, 2015, which is hereby incorporated by reference herein in its entirety. 

What is claimed is:
 1. An ultrasonic motor, comprising: an annular vibrator; and an annular contact member, wherein the annular vibrator comprises: an annular vibrating plate brought into contact with the annular contact member; and a piezoelectric element including a piezoelectric ceramic piece, wherein the annular vibrating plate includes X grooves extending radially, and when an outer diameter of the annular vibrating plate is set to 2R in units of mm, X is a natural number satisfying ((2R/0.85)−5)≤X≤((2R/0.85)+15), wherein a ratio between an average value L_(top) of a length in a circumferential direction on an outer diameter side of a wall region that separates the adjacent grooves from each other and an average value L_(btm) of a length in a circumferential direction on an outer diameter side of the grooves falls within a range of 2.00≤L_(top)/L_(btm)≤2.86, and wherein, when center depths of the X grooves are represented by D₁ to D_(X) in order in the circumferential direction, D₁ to D_(X) take five or more different values.
 2. An ultrasonic motor according to claim 1, wherein the piezoelectric ceramic piece has a Young's modulus at room temperature of 80 GPa or more and 125 GPa or less.
 3. An ultrasonic motor according to claim 1, wherein D₁ to D_(X) have a difference between a maximum value and a minimum value of 5% or more and 25% or less with respect to a maximum thickness T_(dia) of the annular vibrating plate.
 4. An ultrasonic motor according to claim 1, wherein D₁ to D_(X) have a standard depth D_(ave) of 25% or more and 50% or less with respect to a maximum thickness T_(dia).
 5. An ultrasonic motor according to claim 1, wherein the piezoelectric ceramic piece has an annular shape and the piezoelectric element further comprises: a common electrode arranged on a surface of the annular piezoelectric ceramic piece opposed to the annular vibrating plate so as to be sandwiched between the annular piezoelectric ceramic piece and the annular vibrating plate; and a plurality of electrodes arranged on a surface of the annular piezoelectric ceramic piece on a side opposite to the surface on which the common electrode is arranged, the plurality of electrodes comprising two drive phase electrodes, one or more non-drive phase electrodes, and one or more detection phase electrodes, wherein, when a length of one arc, which is obtained by dividing a circumference of a circle that passes through an arbitrary position on a surface of the annular piezoelectric element and shares a center with the annular piezoelectric element by seven, is represented by λ and a circumferential length of the circle is represented by 7λ, the two drive phase electrodes each have a circumferential length of 3λ, and are separated from each other in the circumferential direction by two spacing regions respectively having lengths of λ/4 and 3λ/4 in the circumferential direction, the annular piezoelectric ceramic piece in a region in contact with each of the drive phase electrodes comprises six polarized regions in which polarity is reversed alternately in the circumferential direction, and the one or more non-drive phase electrodes and the one or more detection phase electrodes are arranged in the two spacing regions.
 6. An ultrasonic motor according to claim 1, wherein the outer diameter 2R of the annular vibrating plate is 90 mm or less.
 7. An ultrasonic motor according to claim 1, wherein the annular vibrating plate has an inner diameter 2R_(in) in units of mm, which satisfies a relationship: 2R−16≤2R_(in)≤R−6.
 8. An ultrasonic motor according to claim 5, wherein the annular piezoelectric ceramic piece has an outer diameter smaller than the outer diameter of the annular vibrating plate, and the annular piezoelectric ceramic piece has an inner diameter larger than an inner diameter of the annular vibrating plate.
 9. An ultrasonic motor according to claim 1, wherein the annular vibrating plate has a maximum thickness T_(dia) of 4 mm or more and 6 mm or less.
 10. An ultrasonic motor according to claim 1, wherein the annular vibrating plate is made of an alloy containing 50 mass % or more of steel and 10.5 mass % or more of chromium.
 11. An ultrasonic motor according to claim 1, wherein the piezoelectric ceramic piece comprises a perovskite type metal oxide represented by one of the following general formulae (1) and (2) as a main component, and a content of metal components other than the main component contained in the piezoelectric ceramic piece is 1 part by weight or less in terms of a metal with respect to 100 parts by weight of the perovskite type metal oxide: {M_(h)(Na_(j)Li_(k)K_(1-j-k))_(1-h)}_(1-m){(Ti_(1-u-v)Zr_(u)Hf_(v))_(h)(Nb_(1-w)Ta_(w))_(1-h)}O₃  (1) where M represents at least one kind selected from the group consisting of (Bi_(0.5)K_(0.5)), (Bi_(0.5)K_(0.5)), (Bi_(0.5)Na_(0.5)), (Bi_(0.5)Li_(0.5)), Ba, Sr, and Ca, and 0.06<h≤0.3, 0≤j≤1, 0≤k≤0.3, 0≤j+k≤1, 0<u≤1, 0≤v≤0.75, 0≤w≤0.2, 0<u+v≤1, and −0.06≤m≤0.06; and (Ba_(1-s)Ca_(s))_(α)(Ti_(1-t)Zr_(t))O₃ where 0.986≤α≤1.100, 0.02≤s≤0.30, and 0.020≤t≤0.095.
 12. An ultrasonic motor according to claim 1, wherein D₁ to D_(X) change so as to follow a curve obtained by superimposing one or more sine waves on one another, the grooves reaching a local maximum in 12 or more grooves in the change of the center depth and the grooves reaching a local minimum in 12 or more grooves in the change of the center depth.
 13. An ultrasonic motor according to claim 12, wherein X represents an even number, and of D₁ to D_(X), a depth change of D₁ to D_(X/2) and a depth change of D_(X/2+1) to D_(X) are matched with each other.
 14. An ultrasonic motor according to claim 5, wherein, when a center depth of the groove closest to the detection phase electrode is represented by D_(sen), where sen is a natural number satisfying X≥sen, (D_(sen+1)−D_(sen−1))/D_(sen) is 5% or less.
 15. An ultrasonic motor according to claim 12, wherein, of the grooves reaching the local maximum, the grooves have a center depth that is 1.15 times or more and 1.30 times or less of a standard depth D_(ave) in at least 8 regions.
 16. An ultrasonic motor according to claim 12, wherein, of the grooves reaching the local maximum, a number I of the grooves positioned between the groove having a largest center depth and the groove having a second largest center depth satisfies: I≥X/18.
 17. An ultrasonic motor according to claim 12, wherein 12 to 16 grooves reach the local maximum of the center depth.
 18. An ultrasonic motor according to claim 12, wherein the grooves reaching the local maximum and the grooves reaching the local minimum are not adjacent to each other.
 19. An ultrasonic motor according to claim 1, wherein the outer diameter 2R is 57 mm or more.
 20. An ultrasonic motor according to claim 1, wherein the piezoelectric ceramic piece contains lead in a content of less than 1,000 ppm.
 21. A drive control system comprising at least an ultrasonic motor and a drive circuit electrically connected to the ultrasonic motor, the ultrasonic motor comprising: an annular vibrator; and an annular contact member, wherein the annular vibrator comprises: an annular vibrating plate brought into contact with the annular contact member; and a piezoelectric element including a piezoelectric ceramic piece, wherein the annular vibrating plate includes X grooves extending radially, and when an outer diameter of the annular vibrating plate is set to 2R in units of mm, X is a natural number satisfying ((2R/0.85)−5)≤X≤((2R/0.85)+15), wherein a ratio between an average value L_(top) of a length in a circumferential direction on an outer diameter side of a wall region that separates the adjacent grooves from each other and an average value L_(btm) of a length in a circumferential direction on an outer diameter side of the grooves falls within a range of 2.00≤L_(top)/L_(btm)≤2.86, and wherein, when center depths of the X grooves are represented by D₁ to D_(X) in order in the circumferential direction, D₁ to D_(X) take five or more different values.
 22. A drive control system according to claim 21, wherein the drive circuit comprises a signal generation unit configured to generate a 7th order bending vibration wave in the annular vibrator.
 23. An optical apparatus, comprising at least an ultrasonic motor, a drive circuit electrically connected to the ultrasonic motor, and an optical element dynamically connected to the ultrasonic motor, the ultrasonic motor comprising: an annular vibrator; and an annular contact member, wherein the annular vibrator comprises: an annular vibrating plate brought into contact with the annular contact member; and a piezoelectric element including a piezoelectric ceramic piece, wherein the annular vibrating plate includes X grooves extending radially, and when an outer diameter of the annular vibrating plate is set to 2R in units of mm, X is a natural number satisfying ((2R/0.85)−5)≤X≤((2R/0.85)+15), wherein a ratio between an average value L_(top) of a length in a circumferential direction on an outer diameter side of a wall region that separates the adjacent grooves from each other and an average value L_(btm) of a length in a circumferential direction on an outer diameter side of the grooves falls within a range of 2.00≤L_(top)/L_(btm)≤2.86, wherein, when center depths of the X grooves are represented by D₁ to D_(X) in order in the circumferential direction, D₁ to D_(X) take five or more different values, and wherein the drive circuit comprises a signal generation unit configured to generate a 7th order bending vibration wave in the annular vibrator.
 24. An annular vibrator, comprising: an annular vibrating plate; and a piezoelectric element including a piezoelectric ceramic piece, wherein the annular vibrating plate includes X grooves extending radially, and when an outer diameter of the annular vibrating plate is set to 2R in units of mm, X is a natural number satisfying ((2R/0.85)−5)≤X≤((2R/0.85)+15), wherein a ratio between an average value L_(top) of a length in a circumferential direction on an outer peripheral side of a wall region that separates the adjacent grooves from each other and an average value L_(btm) of a length in a circumferential direction on an outer peripheral side of the grooves falls within a range of 2.00≤L_(top)/L_(btm)≤2.86, and wherein, when center depths of the X grooves are represented by D₁ to D_(X) in order in the circumferential direction, D₁ to D_(X) take five or more different values. 